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© IWA Publishing 2014 Journal of Water Supply: Research and Technology—AQUA
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Quantifying bacterial biomass fixed onto biological activated carbon (PAC and GAC) used in drinking water treatment Céline Stoquart, Benoit Barbeau, Pierre Servais and Gabriela A. Vázquez-Rodríguez
ABSTRACT Hybrid processes coupling the use of powder activated carbon (PAC) with membrane filtration for drinking water production are emerging as promising alternatives to conventional technologies due to their enhanced control of dissolved contaminants. The quantification of biomass colonizing PAC is crucial for modeling, designing control strategies and improving the overall performance of these processes. The aim of this study was to examine the applicability of several common methods developed for colonized granular activated carbon (GAC) to PAC. Six analytical methods (based on the measurement of proteins, polysaccharides, heterotrophic plate counts, potential glucose respiration, bacterial ATP and a potential acetate uptake rate, which is proposed herein) were compared. The results showed that the rates of glucose respiration and of acetate consumption could be used interchangeably. Proteins were also an interesting alternative for on-site measurements. It was concluded that biological PAC-based processes sustained a level of heterotrophic activity similar to or greater than that observed in GAC biofilters. Key words
| biofilters, drinking water, extracellular polymeric substances, microbial activity,
Céline Stoquart Benoit Barbeau Gabriela A. Vázquez-Rodríguez (corresponding author) NSERC Industrial Chair on Drinking Water, Department of Civil, Mining and Geological Engineering, École Polytechnique de Montréal, NSERC-Industrial Chair in Drinking Water, C.P. 6079, Succursale Centre-Ville, Montréal, QC, Canada H3C 3A7 E-mail: g.a.vazquezr@gmail.com, gvazquez@uaeh.edu.mx Gabriela A. Vázquez-Rodríguez Permanent address: Centro de Investigaciones Químicas, Universidad Autónoma del Estado de Hidalgo, Carr. Pachuca-Tulancingo km. 4.5, 42184 Mineral de la Reforma, Hgo., Mexico Pierre Servais Écologie des Systèmes Aquatiques, Université Libre de Bruxelles, Campus de la Plaine, CP 221, Boulevard du Triomphe, B-1050 Brussels, Belgium
substrate uptake rates
INTRODUCTION Biological filters have been used extensively for the pro-
non-adsorptive supports (e.g. sand or anthracite) (Wang
duction of drinking water in North America and Europe.
et al. ). Moreover, both the irregular surface and the
Some of their advantages include the biological stabilization
porous structure of GAC protect the biomass against shear
of treated water via the removal of dissolved organic matter
forces and toxic loads (Chaudhary et al. ; Herzberg
and ammonia, a decrease in chlorine demand and the for-
et al. ).
mation of fewer disinfection by-products. Currently, these
Recent developments in membrane technologies for
processes are becoming increasingly important due to the
drinking water production include the integration of
rise of green technologies and the emergence of new con-
powder activated carbon (PAC) in processes referred to as
taminants that may be amenable to biodegradation, such
hybrid membrane processes (HMPs) (Stoquart et al. ).
as several pharmaceuticals, taste and odor compounds and
PAC targets dissolved compounds that are not retained by
cyanotoxins (Brown ). Granular activated carbon
low-pressure membranes. It offers faster adsorption rates
(GAC) is the preferred medium for biological filters because
than GAC (Yener et al. ) and can be injected and recov-
it offers more sites for microbial attachment than
ered continuously from a slurry-type suspension. This
doi: 10.2166/aqua.2013.101
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Quantifying bacterial biomass fixed onto biological activated carbon
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configuration offers high flexibility to address sudden source
challenges. One promising alternative substrate is acetate,
water quality variations by simply adjusting the age of the
a ubiquitous compound that can be used as a substrate by
PAC slurry to control adsorption performance (Stoquart
almost all eubacterial and fungal cells (Wang et al. ).
et al. ).
For instance, the abundance of acetate-utilizing bacteria
When using activated carbon (AC), biodegradable com-
has been estimated microautoradiographically as 47–93%
pounds can be removed by adsorption, biodegradation or a
of the total bacteria in wastewater-activated sludge (Nielsen
combination thereof. Within the HMP, the relative impor-
& Nielsen ). In addition, acetate is a common ozonation
tance of both mechanisms is intimately related to the age
by-product
of the PAC slurry. Assessing the relative importance of
biodegraders are likely to be present in drinking water biofil-
both mechanisms is paramount for modeling the process
ters. Moreover, acetate is poorly adsorbable onto GAC
and thus optimizing its performance. Therefore, reliable
(Moteleb et al. ) and PAC (Stoquart et al. ), which
techniques for evaluating microbial colonization onto PAC
minimizes potential bias in the evaluation of the acetate
are required.
uptake rate. Thus, measuring the potential acetate uptake
Several methods have been developed to evaluate bacterial biomass fixed on GAC. As proposed by Lazarova
(Urfer
&
Huck
).
Hence,
acetate-
(PAU) rate could be an interesting alternative for evaluating active bacterial biomass fixed on solid media.
et al. (), they can be classified as either non-destructive
To the best of our knowledge, no published studies have
or destructive (i.e. techniques that disrupt the biofilm). Non-
aimed to quantify the biomass developed on the PAC sur-
destructive methods include direct microscopy and tech-
face from drinking water treatment processes. This work
niques based on the measurement of specific activities, such
was thus conducted to evaluate the applicability of several
as the potential glucose respiration (PGR) (Servais et al.
existing analytical methods (i.e. the assessment of PGR,
), the overall oxygen consumption (Urfer & Huck )
HPC, ATP and EPS) and to propose a new method based
or the potential nitrifying activity developed to estimate the
on measuring PAU rates for characterizing heterotrophic
autotrophic nitrifying biomass (Kihn et al. ). On the
biomass on biological PAC obtained from two hybrid pilot
other hand, destructive methods, which require detaching
membrane processes. The results obtained for PAC were
the biomass from the support media, include total cell count-
also compared with those measured on a biological GAC
ing
by
epifluorescence
(Nishijima
),
the
(BAC) sample collected from a full-scale biofilter. Finally,
enumeration of heterotrophic plate counts (HPC) (Camper
the results obtained from the six tested analytical methods
et al. a, b) and the measurement of compounds related
were compared.
et
al.
to the viable biomass, such as phospholipids (Wang et al. ) and ATP (Velten et al. ), and the biofilm density, such as the concentrations of polysaccharides (Quintelas
MATERIALS AND METHODS
et al. ) and proteins (Drogui et al. ; Papineau et al. ) in extracted extracellular polymeric substances (EPS).
Description of samples
All the aforementioned techniques have only been applied to GAC, not biological PAC. Non-destructive
AC characteristics
methods are the most interesting because the detachment of the biomass is undesirable due to issues such as incom-
Three types of wood-derived AC commercialized by Pica™
plete recovery and the impact of the procedure on cellular
(Picahydro LP 39, Picahydro L30-260 and Picabiol 2) were
integrity (Lazarova et al. ). Amongst the non-destructive
tested; the non-colonized media are referred to as NP25,
methods, PGR allows the biomass potentially responsible
NP200 and NGAC, respectively. NP25 and NP200 are
for the removal of biodegradable compounds to be evalu-
PAC with median particle sizes of 15–35 and 210–260 μm,
ated. However, the PGR method requires the use of a
respectively. NGAC has a median particle size of 500–
radiolabeled substrate (i.e.
14
C-glucose), which is expensive,
not always readily available and may pose logistical
700 μm. Their iodine numbers vary between 900 and 1,000 mg/g.
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(with NGAC-type characteristics; H ¼ 180 cm). The empty
AC colonization
bed contact time in the filter ranged from 20 to 30 min The colonization of PAC was carried out in four parallel
depending on the water demand. A summary of the characteristics of the five colonized
HMP pilots operating under two configurations. The pilots were fed with coagulated-settled river water (Des Mille-Iles
AC samples is presented in Table 1.
River, Laval, Canada). The average main influent characteristics
were
2.9 mg
DOC/L,
0.23 mg
BDOC/L
and
Biomass measurements
154 μg N-NH3/L. In the first configuration (PAC/UF), the PAC treatment was integrated to a submerged ultrafiltration
The biomass measurements were performed on the same day
(UF) unit described in detail by Léveillé et al. (). Two
for all analytical techniques and sample types tested (i.e. the
PAC/UF reactors were filled with NP25. In the first AC/
five colonized samples and the three virgin samples). The
UF reactor (P7-5), a PAC concentration of 5 g dry weight
virgin samples (NP25, NP200 and NGAC) were used as con-
(dw)/L, a solids retention time (SRT) of 7 days and a hydrau-
trols. Before any experiment, 10 g dw of each of the virgin AC
lic residence time (HRT) of 69 min were maintained. In the
samples was humidified overnight at room temperature in 1 L
second PAC/UF pilot (P60-10), the PAC concentration, the
of Milli-Q water. The pH of the slurry (approximately 3) was
SRT and the HRT were 10 g dw/L, 60 days and 77 min,
raised to 7.0 by adding 1 M NaOH. The colonized PAC slur-
respectively.
ries (P7-5, P60-10, P67-1 and P67-5) were withdrawn at the
In the second configuration (PAC þ UF), water was fed
same time from the four reactors. All the PAC samples (colo-
into two parallel stirred-tank reactors filled with NP200,
nized and virgin) were recovered by filtration on a Grade 41
which was maintained inside the reactors using a 55–
paper filter (Whatman). Finally, the BAC sample was col-
85 μm sieve. The effluent water was then fed into the UF
lected from the surface of the biofilter.
modules. The PAC concentrations within the reactors were 1 g dw/L (P67-1) and 5 g dw/L (P67-5). Unlike the
PAU rate
PAC/UF configuration, both reactors were operated continuously without any PAC replacement (i.e. with variable
According to Monod kinetics, the rate of substrate depletion
SRT). At the sampling time, an SRT of 67 days had been
(dS/dt) and the specific microbial growth rate (μ) can be
reached in both PAC þ UF reactors.
expressed by Equations (1) and (2), respectively:
The BAC samples were obtained from the surface of a full-scale dual media filter (80 m2 surface area) composed of layers of sand (D10 ¼ 0.45 mm, H ¼ 15 cm) and GAC
Table 1
|
dS μX ¼ dt Y
(1)
Biological AC sample characteristics
Concentration in the reactor Sample IDa
Type of carbon
Median diameter (μm)
Pilot unit
Carbon used for starting up the pilot
SRT (days)
b
(g dw/L)
P7-5
PAC
15–35
PAC/UF
NP25
7
5
P60-10
PAC
15–35
PAC/UFb
NP25
60
10
P67-1
PAC
210–260
PAC þ UFc
NP200
67
1
P67-5
PAC
210–260
PAC þ UFc
NP200
67
BAC
GAC
500–700
a
Biological GAC
NGAC
N.A.
The first number refers to the age (d) of the carbon and the second number refers to the PAC concentration (g dw/L) within the contactor. Hybrid membrane process with integrated AC treatment.
b c
Hybrid membrane process with AC pretreatment.
d
N.A.: not available.
5 d
350
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μ ¼ μmax
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The acetate concentration was determined in duplicate
S S þ KS
(2)
samples by ion chromatography (Dionex Corporation, Sunnyvale, USA). The apparatus was equipped with an
where X is the biomass concentration, Y is the growth yield,
IonPac AS18 column and suppressed conductivity detec-
μmax is the maximum specific growth rate and KS is the half-
tion. An EluGen® EGC-KOH cartridge was used as the
saturation constant. Equation (3) is obtained by substituting
eluent. The limit of detection, the limit of quantification,
Equation (2) into Equation (1) as follows:
the reproducibility and the accuracy of this method are 0.0159 mg/L, 0.0530 mg/L, 3 and 4.5%, respectively. The
dS μ X S ¼ max dt Y S þ KS
PAU rates were calculated from the initial slope of the acet(3)
ate content obtained by linear regression, normalized per gram of AC dw in the assay. These rates are expressed as
If S > >Ks, Equation (3) can be simplified as:
specific acetate uptake rates in mmol Na-acetate per g AC dw per hour. Regressions made to calculate PAU rates
dS μ X ¼ max dt Y
(4)
qS, the specific substrate removal rate, is defined by
were always significant (p < 0.05) with R 2 > 0.96, except for P7-5 (R 2 ¼ 0.61) and P60-10 (R 2 ¼ 0.72). PGR rate
Equation (5): The production of dS qS ¼ X dt
(5)
CO2 due to the mineralization of
14
C-
glucose under saturating conditions was measured according to the method of Servais et al. (). This method uses
Thus, Equation (4) can be rewritten to give Equation (6): qS ¼
14
μmax Y
(6)
a similar fundamental approach to the PAU method, although radioactive glucose replaces acetate as a substrate and mineralization (CO2 production) is measured rather than substrate consumption. A mixture containing
14
C-
glucose and non-radiolabeled glucose was prepared to Equation (6) shows that under substrate saturating con-
obtain a final glucose concentration of 1 mM and a radioac-
ditions (i.e. S > >Ks), the substrate is removed following
tivity of 0.1–1 μCi/mL. One milliliter of this mixture was
zero-order kinetics during the first few hours of incubation.
added to 1 g ww of AC in a penicillin flask closed with a
Thus, qS (hereafter referred to as the PAU rate) can be con-
rubber septum. After 3 h of incubation at 20 C, the
W
sidered an estimate of the microbial biomass fixed on the
sample was acidified by adding 2 mL of 10% H2SO4 through
media because the uptake rate and biomass are proportional
the septum. Samples were bubbled for 10 min to extract the
(Equation (6)).
CO2, which was trapped in a mixture of Carbo-SorbE
The PAU rates were estimated in 1 L beakers containing
(Perkin Elmer) and PermafluorEþ (Perkin Elmer, 1:4 v/v).
500 mL of test medium. The latter contained a saturating
The radioactivity was determined by liquid scintillation
initial concentration of sodium acetate (15 mg Na-acetate/L,
with a Packard Tri-Carb (TR-1600) scintillation counter.
equivalent to 4.4 mg C/L) and was supplemented with
The amount of glucose mineralized was measured in tripli-
NH4Cl (0.65 mg N/L) and phosphate buffer (0.06 mg P/L).
cate and expressed as nmol glucose per g AC dw per hour.
After adding 10 g wet weight (ww) of AC, the slurries were W
maintained at 20 C under agitation at approximately
Heterotrophic plate counts
150 rpm using a magnetic stirrer. Samples were withdrawn periodically by filtering 40 mL of slurry through a 0.45 μm
For each sample, 1 g ww of the AC sample was homogen-
polyethersulfone membrane previously rinsed with 1 L of
ized in a blender at 16,000 rpm and 4 C for 3 min with a
Milli-Q water.
mixture
W
of
Zwittergent
(10–6 M),
EGTA
(ethylene
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glycol-bis-(β-aminoethyl ether)-N,N,N0 ,N0 -tetraacetic acid,
supernatants were recovered and filtered through sterile
10–3 M), Tris buffer (0.01 M, pH 7.0) and 0.1% peptone
0.45 μm pore size membranes.
(Camper et al. a). The culturable cells were analyzed
The protein content of the extracts was determined
in duplicate on decimal dilutions using the membrane fil-
using a bicinchoninic acid method-based commercial kit
tration technique (9215 D Standard Methods, (APHA
(Pierce© BCA Protein Assay Kit, Thermo Scientific, USA)
)). The membrane filters were incubated on R2A agar
with a bovine serum albumin (BSA) standard. The results
W
at 20 C in the dark. After 7 days, the HPCs were determined
were expressed in mg of proteins (equivalent BSA) per g
and expressed in CFU per g AC dw.
of AC dw or in mg C per g of AC dw, knowing that carbon represents 45% of the mass of BSA. The polysaccharides were analyzed by the phenol-sulfuric acid method using
Bacterial ATP
glucose as a standard (Dubois et al. ). The results were ®
An ATP detection kit was used (Profile -1 Reagent Kit, New
expressed in mg polysaccharides (equivalent glucose) per g
Horizons Diagnostics, USA). The kit consisted of a microlu-
of AC dw or mg C per g of AC dw, knowing that carbon rep-
minometer, filtration devices (0.4 μm pore diameter), a
resents 40% of the molecular weight of glucose. The total
lysing reagent for non-bacterial ATP (somatic releasing
amount of EPS was obtained by summing the concen-
agent, SRA) and a second reagent ensuring both bacterial
trations of proteins and polysaccharides (both expressed as
lysis and leaching of bacterial ATP (bacterial releasing
mg C per g of AC dw).
agent, BRA). Prior to the analysis, the samples were homogenized, just as for the measurement of HPC, and then
Dry weight
10-fold diluted in phosphate buffer to minimize ATP adsorption on AC. After the filtration of 225 μL of the suspension in
The virgin and biological AC were dried for 24 h at 105 C
the filtration device, 60 μL of SRA was added and evacuated
according to the standard method 2540 B (APHA ) to
twice to discard the non-bacterial ATP. In a second step,
obtain the dry weights of samples. The results of all microbio-
60 μL of BRA was added to the sample in the Filtravette
logical measurements were then expressed per g of AC dw.
W
device, filtered and recovered. Finally, 25 μL of the filtrate was mixed with 225 μL of reconstituted luciferin-luciferase reagent (Molecular Probes®, USA) in a new Filtravette
RESULTS AND DISCUSSION
device and the relative luminescence units were recorded. Positive controls were obtained by adding two standards
The analytical methods described previously were applied to
with high concentrations of ATP (ranging from 0.8 to
quantify the biomass fixed onto AC samples. Concerning
2.7 μg ATP/L) to the samples. The results were compared
biological PAC samples, different levels of biomass density
to a standard curve (0.01–3 ng ATP/L) and expressed as
were expected because the colonization was carried out
ng ATP per g AC dw. No replicates were made.
under variable PAC ages and concentrations within the reactors. First, P7-5 and P67-5 were two PAC samples colonized at the same concentration in the pilot reactor (i.e.
EPS: polysaccharides and proteins
5 g dw/L). Although these two PAC had distinctive sizes, EPS were extracted in duplicate using approximately 2 g ww
no significant differences with respect to biomass density
of sample according to the method proposed by Liu & Fang
were expected due to this factor (Markarian et al. ).
(). The samples were resuspended in 10 mL of phos-
However, higher ages (67 vs. 7 days) were expected to
phate buffer supplemented with 60 μL of formaldehyde
lead to higher biomass densities for AC colonized under
W
(36.5% v/v) and then incubated at 4 C for 1 hour under agi-
equivalent conditions. Second, two reactors were operated
tation. After the addition of 4 mL of 1 M NaOH, the samples
with the same PAC age (67 days) but variable PAC concen-
W
were incubated for 3 h at 4 C. Next, the slurries were centriW
fuged twice at 12,000 g and 4 C for 15 min. Finally, the
trations inside the reactor (P67-1 and P67-5). In that case, equivalent colonization (expressed per g of AC dw) is not
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expected; Markarian et al. () noted that the develop-
after 24 h of contact (data not shown). This finding confirms
ment of biomass on biological PAC is limited by substrate
that any acetate removal is due to biological activity.
availability rather than the available colonization surface.
The initial acetate concentration applied in the assays
Consequently, it was hypothesized that PAC colonized at a
was approximately 3-fold higher than Ks (the value
lower concentration in the pilot reactor would support a
embedded in Biowin™ software is 5 mg/L). This concen-
higher biomass density on its surface. The results gathered
tration led to the expected zero-order kinetics for acetate
from each analytical method are presented and discussed
removal when the biomass growth is negligible compared
separately as follows.
to the biomass initially present on the AC. Hence, all colonized samples removed acetate at a constant rate during the first 4–6 h (Figure 1).
PAU rates
Figure 2(a) depicts the results of the PAU tests. The No decrease in the acetate concentration was observed in
lowest PAU rate was found for the P7-5 sample, which
the experiments conducted with virgin materials, even
was expected to have the lowest level of bacterial colonization due to the short SRT of the reactor (7 days), whilst the maximum PAU rate was measured for the P67-1 sample (colonized at the highest SRT). Actually, the PAU rate measured for the P67-1 sample was not significantly different from that measured for the biological GAC filter (i.e. the BAC sample). Sample P67-5 presented a statistically significantly higher PAU rate than sample P7-5 (p < 0.05) confirming that higher SRT led to a higher active biomass on the PAC surface. In addition, the PAC samples colonized at a lower PAC concentration (P67-1) had a statistically significantly higher PAU rate than its counterpart colonized at 5 g/L (P67-5) (p < 0.05). In this way, the positive effect of a high substrate availability on the activity of the biomass fixed onto PAC appears to be confirmed too. Based on these preliminary results, the measurement of PAU rates is a promising method. This finding should be
Figure 1
|
Acetate uptake by virgin and colonized samples of AC. The symbols represent the experimental results, and the lines represent the data from the linear regression.
Figure 2
|
confirmed by validating this method with a wider set of samples, including more BAC samples. In addition,
(a) PAU rates of biological AC samples. Error bars represent the standard errors of the regression slopes used for calculating PAU rates. (b) PGR rates of biological AC samples. Error bars represent standard deviations. Solid lines (
) represent the background values measured on the corresponding virgin samples.
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monitoring the depletion of acetate in the first hours of the
samples ranged from 17.7 to 69.4 μg C/cm3, whereas a bio-
assay in short time intervals is necessary for properly moni-
mass of 38.6 μg C/cm³ was measured at the surface of the
toring the zero-order kinetics.
biological filter (sample BAC). This value is higher than the PGR measured previously by Niquette et al. () at the top of the same full-scale GAC biofilter (20 μg C/cm3).
PGR rates
This difference could be partly explained by the temperature Figure 2(b) presents the PGR rates measured on colonized
in the filter (16 C in our case vs. 11 C measured pre-
AC. The background values obtained for the virgin PAC
viously). In an another study reporting the colonization of
were between 0.07 and 0.44 nmol/g AC dw · h. These
a biofilter at 16 C, the PGRs were comprised between 2.5
values were not significantly different from one another
and 10.9 μg C/cm3 (Servais et al. ), while an average
(p > 0.05) and were considerably lower (120- to 1,900-fold)
value of 4.7 μg C/cm3 was proposed as representative of
than the values obtained for the colonized materials. There-
the fixed biomass in a GAC biofilter at steady state (Servais
fore, the PGR values shown in Figure 2(b) and elsewhere in
et al. ). The higher biomass densities observed on our
this paper were not corrected for the background
PAC samples are most likely explained by the amount of
measurement.
support area available for the colonization and the nutrients
W
W
W
The PGR of the sample P7-5 (43.1 nmol/g AC dw · h)
limitation. Indeed, the PAC samples were colonized at low
was significantly different from the virgin samples (p <
concentrations (i.e. 1 to 10 g/L), whereas a larger mass of
0.05). The PGR rates obtained for the samples with higher
GAC typically provides support for the colonization at the
SRT (i.e. at least 60 days) led to the same conclusions as
surface of a BAC filter. In addition, the biomass densities
for the PAU method, with P60-10 being more colonized
measured on BAC come from second-stage filters, while
than P7-5 and P67-1 being more colonized than P67-5. All
our PAC was colonized as a first-stage process. Niquette
the samples with a high SRT presented a PGR not signifi-
et al. () observed a similar trend (i.e. higher colonization
cantly different from the BAC sample.
in first- as opposed to second-stage BAC filters). As
To compare our results with the values of PGR found in 3
the literature (usually reported as μg of C-biomass/cm ), the
described earlier, this result is explained by the higher nutrient loading offered in first-stage processes.
PGR rates were converted by considering a mean density value of 1.33 g of wet AC per cm3 and a correspondence
Heterotrophic plate counts
factor of 1.1 μg C of bacterial biomass per nmol of glucose respired per hour. This last value was originally obtained
The results of the analysis of HPC are presented in Figure 3(a).
by calibrating the radiochemical method with bacteria
The densities of HPC on biological PAC ranged from
washed off from GAC filter samples and enumerated by epi-
4.2 × 107 to 3.0 × 108 CFU/g PAC dw, whereas the value
fluorescence microscopy (Servais et al. ). Following this
for the BAC sample was 3.3 × 107 CFU/g GAC dw. The
conversion, our PGR values obtained for the colonized PAC
results obtained are of the same order of magnitude as the
Figure 3
|
(a) HPC in biological AC samples. Error bars represent standard deviations. (b) Bacterial ATP contents in biological AC samples. B.D.: Below detection limit.
8
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literature values for BAC. However, no further comparison
capacity of PAC is an important concern when using ATP
can be drawn. The culture conditions (i.e. culture medium
and future work should aim for an improved separation of
and incubation temperature) applied were indeed highly
the biofilm from the PAC particles before conducting the
variable, leading to potentially large variations in the HPC
ATP analysis.
8
results. LeChevallier et al. () measured 10 CFU/g
For colonized GAC, the measured value (58.9 ng ATP/g
GAC on a TLY medium, Camper et al. (b) measured
BAC dw or 14.07 ng ATP/g BAC ww) was lower than the
5 × 107 CFU/g GAC after incubating at 35 C, and Niemi
usual ATP contents. Niemi et al. () measured 0.5–
7
0.7 nmol ATP/g GAC dw (equivalent to 254–355 ng/g
W
8
et al. () measured 6 × 10 to 10 CFU/g GAC dw after W
GAC dw), while Velten et al. () measured 1,170 ng
incubating at 25 C. As mentioned before, the detachment of bacterial cells
ATP/g GAC ww at the surface of a fully colonized biofilter.
from the support medium is critical when using the plate
In the former case (Niemi et al. ), a prior extraction of
count procedure to assess biomass density. In this study,
the ATP had been carried out, thereby indicating that the
the higher values of culturable cells obtained for biological
method used herein could most likely be improved by
PAC may be the result of the homogenization step being
including an ATP extraction step before the addition of the
more efficient for smaller particles. Indeed, the shear
luciferin-luciferase complex.
stress is inversely proportional to the cross-sectional area of the material with area parallel to the applied force vector.
EPS: polysaccharides and proteins
Bacterial ATP
The results of the analysis of extracellular proteins and polysaccharides are presented in Figure 4(a). The proteins
The results obtained for the bacterial ATP are presented in
ranged from 6.7 to 14.0 mg/g PAC dw and 8.1 mg/g BAC
Figure 3(b). The ATP concentration measured on sample
dw (or 1.9 mg/g BAC ww). The results obtained for the
P7-5 was below the detection limit, whereas sample P60-
BAC were lower than those obtained in laboratory-scale
10 presented an ATP concentration of only 5 ng ATP/g
GAC columns removing microcystin-LR from drinking
PAC dw. Samples P67-5 and P67-1 presented ATP concen-
water (17.2–37.2 mg/g GAC ww) (Drogui et al. ). Poly-
trations of 39 and 80 ng ATP/g PAC dw, respectively.
saccharides were present at lower concentrations than
These results may have been biased by the impact of residual
proteins: 1.0–3.6 mg/g PAC dw and 5.1 mg/g BAC dw.
adsorption. Positive controls confirmed that ATP readily
Figure 4(b) presents the total EPS measurements as well
adsorbed onto PAC particles. Luminescence losses ranging
as the polysaccharide-to-protein ratio. The calculated poly-
from 70 to 99% were detected after the addition of an
saccharide-to-protein ratios were similar in the various
ATP standard to the PAC. Thus, the residual adsorption
samples of biological PAC with SRT of at least 67 days
Figure 4
|
(a) Measured ( EPS, (
) proteins, (
) background proteins, (
) background total EPS and (
) polysaccharides and (
) background polysaccharides in biological AC samples. (b) Measured (
) polysaccharide-to-protein ratio in biological AC samples. Error bars represent standard deviations.
) total
9
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Quantifying bacterial biomass fixed onto biological activated carbon
(0.22 ± 0.04). The youngest PAC (i.e. P7-5) had a lower
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Comparison of methods
ratio (0.13 ± 0.002), whereas the GAC sample cumulated the greatest amount of polysaccharides (0.56 ± 0.1). As a
A comparison was performed by considering all the tested
reference, higher polysaccharide-to-protein ratios have
methods except for the ATP method, which remains to be
been associated with higher SRT in activated sludge
optimized. Figure 5 compares the results obtained with
(Massé et al. ; Satyawali & Balakrishnan ),
our reference method (i.e. PGR) and the results of the
which is consistent with our results. In fact, the relative
PAU rates, log HPC and the contents of proteins, polysac-
abundance of polysaccharides over proteins has been
charides and total EPS. The corresponding correlation
explained by the slower hydrolysis rate of polysaccharides
matrix is presented in Table 2. This matrix confirms that
(Massé et al. ). The increase in the polysaccharide-to-
the results of the PAU tests were significantly correlated
protein ratios at high SRT could also arise from a higher
with the PGR values (r ¼ 0.82), suggesting the possibility of
polysaccharide production, which would increase the bac-
using either technique interchangeably. In addition, there
terial adhesion to AC. Indeed, polysaccharides are widely
were strong correlations between methods based on poten-
recognized as key in mediating both cell-to-cell interactions
tial activity and the EPS analysis (r > 0.75). The total EPS
and cell attachment to supports (Tay et al. ). As poly-
and proteins were better correlated with the PGR method
saccharides tend to accumulate (cf. low hydrolysis rate),
(r ¼ 0.92 and 0.89, respectively), whereas the polysacchar-
this technique may lead to an improper assessment of AC
ides results were better correlated with the PAU data
microbial colonization for high SRT. In particular, compar-
(r ¼ 0.96).
ing fully colonized samples with different SRT is not
All of the methods investigated differentiated between
possible because old AC should lead to higher polysacchar-
the colonized AC and the corresponding virgin material
ides contents for the same amount of active biomass.
(p < 0.05) for all of the samples tested. As confirmed by
However, by considering the total amount of EPS (i.e. the
the background measurements, the EPS methods were the
sum of proteins and polysaccharides) as presented in
least sensitive (see background measurements on Figures 4(a)
Figure 4(b), similar trends as the one observed for the
and (b)). In contrast, the PGR method was the most sensitive
potential activity-based methods (i.e. PAU and PGR) were
method. Indeed, by raising the ratio of the radioactive
obtained.
specific activity of the glucose solution added to the AC
Figure 5
|
PAU rate, log HPC, proteins, polysaccharides and total EPS as a function of the PGR rate measured on biological and virgin AC samples.
10
C. Stoquart et al.
Table 2
|
|
Quantifying bacterial biomass fixed onto biological activated carbon
Correlation matrix (I-values, p < 0.05) between the results obtained with the PAU, PGR, proteins, polysaccharides, total EPS and log HPC methods
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while the ATP and the EPS measurements allowed the evaluation of not only the heterotrophic bacteria, but the entire bacterial and non-bacterial biomass. These differences
PAU
PGR
Proteins
Polysac.
Total EPS
Log HPC
PAU
1
0.82
0.80
0.96
0.88
0.72
should be kept in mind and the investigation of the
PGR
0.82
1
0.89
0.84
0.92
0.87
microbial communities established at the surface of the
Proteins
0.80
0.89
1
0.75
0.98
0.81
AC under variable SRT would provide additional insight
Polysac.
0.96
0.84
0.75
1
0.85
0.66
on the results of the different methods applied in this study.
Total EPS
0.88
0.92
0.98
0.85
1
0.89
Log HPC
0.72
0.87
0.81
0.66
0.89
1
CONCLUSIONS
*Polysac.: Polysaccharides.
The results from PAU, PGR, EPS and HPC methods were (by increasing the proportion of radioactive glucose in this
strongly correlated. The PAU rate is a promising method
solution), the sensitivity can be easily improved.
to assess the bacterial activity on PAC and GAC. However,
Among biological PAC samples, P67-1 carbon exhibited
it should be validated for a wider set of colonized AC
the maximum results of all the six analytical methods, which
samples. Because protein content is well correlated with
were higher than those presented by the P67-5 sample. The
the PAU and PGR results, it would be a good surrogate
enhanced microbial colonization of P67-1 carbon might be
for on-site biomass measurements. A high SRT increased
due to the higher substrate availability that prevailed in
the activity of heterotrophic biomass and the amount of
this reactor (with the lowest PAC concentration). No statisti-
EPS associated to the biofilms. Finally, it was concluded
cally significant difference was found between the P67-1 and
that heterotrophic activities comparable to BAC filters can
BAC samples using the PGR method (p > 0.05), although
be obtained in biological PAC-based drinking water systems.
this finding may be attributed to the considerable standard deviation of the BAC results (i.e. 41%). The total EPS method indicated that the P67-1 sample was more colonized
ACKNOWLEDGEMENTS
than the BAC sample, whereas the opposite was true for the PAU method. These results support the idea that the bio-
The authors would like to thank the outstanding technical
mass of a PAC-based process is as active as the biomass at
support of Jacinthe Mailly, Jörg Winter, Julie Philibert,
the surface of a conventional biological GAC filter for drink-
Marcellin Fotsing, Mélanie Rivard, Mireille Blais and Yves
ing water treatment.
Fontaine. This work was completed at the Industrial-
Both potential activity-based methods (PGR and PAU)
NSERC Chair in Drinking Water of École Polytechnique
could be used to improve the modeling of DOC and
de Montréal with the financial support of its partners,
BDOC removal as well as the control strategies and the
namely the City of Montreal, John Meunier, Inc., and the
overall performance of biological processes used in drinking
City of Laval.
water production. The protein measurements were highly correlated
with
the
potential
activity
methods
(see
Table 2). From an operational viewpoint, the protein analysis is the least cumbersome and time-consuming of all techniques tested during this project. It could be used as an easily measurable surrogate for monitoring the microbial activity on biological AC in water treatment plants. It is worth highlighting that, amongst the methods tested, the PAU and PGR rates and HPC methods were designed to provide data on the heterotrophic biomass
REFERENCES APHA Standard Methods for the Examination of Water and Wastewater, 22nd edn. American Public Health Association, American Waterworks Association, Water Environment Federation, Washington, DC. Brown, J. C. Biological treatments of drinking water. Bridge 37, 30–36. Camper, A. K., LeChevallier, M. W., Broadaway, S. C. & McFeters, G. A. a Evaluation of procedures to desorb
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bacteria from granular activated carbon. J. Microbiol. Methods 3, 187–198. Camper, A. K., LeChevallier, M. W., Broadaway, S. C. & McFeters, G. A. b Growth and persistence of pathogens on granular activated carbon filters. Appl. Environ. Microbiol. 50, 1378–1382. Chaudhary, D. S., Vigneswaran, S., Jegatheesan, V., Ngo, H. H., Moon, H., Shim, W. G. & Kim, S. H. Granular activated carbon (GAC) adsorption in tertiary wastewater treatment: experiments and models. Water Sci. Technol. 47 (1), 113–120. Drogui, P., Daghrir, R., Simard, M. C., Sauvageau, C. & Blais, J. F. Removal of microcystin-LR from spiked water using either activated carbon or anthracite as filter material. Environ. Technol. 33, 381–391. Dubois, M., Gilles, K. A., Hamilton, J. K., Rebers, P. A. & Smith, F. Colorimetric method for determination of sugars and related substances. Analyt. Chem. 28, 350–356. Herzberg, M., Dosoretz, C. G., Tarre, S. & Green, M. Patchy biofilm coverage can explain the potential advantage of BGAC reactors. Environ. Sci. Technol. 37, 4274–4280. Kihn, A., Laurent, P. & Servais, P. Measurement of potential activity of fixed nitrifying bacteria in biological filters used in drinking water production. J. Ind. Microbiol. Biotechnol. 24, 161–166. Lazarova, V., Pierzo, V., Fontvielle, D. & Manem, J. Integrated approach for biofilm characterization and biomass activity control. Water Sci. Technol. 29 (7), 345–354. LeChevallier, M. W., Hassenauer, T. S., Camper, A. K. & McFeters, G. A. Disinfection of bacteria attached to granular activated carbon. Appl. Environ. Microbiol. 48, 918–923. Léveillé, S., Carrière, A., Charest, S. & Barbeau, B. PAC membrane bioreactor as an alternative to biological activated carbon filters for drinking water treatment. J. Water Suppl. Res. Technol. AQUA 62, 23–34. Liu, H. & Fang, H. H. P. Extraction of extracellular polymeric substances (EPS) of sludge’s. J. Biotechnol. 95, 249–256. Markarian, A., Carrière, A., Dallaire, P.-O., Servais, P. & Barbeau, B. Hybrid membrane process: performance evaluation of biological PAC. J. Water Suppl. Res. Technol. AQUA 59, 209–220. Massé, A., Spérandio, M. & Cabassud, C. Comparison of sludge characteristics and performance of a submerged membrane bioreactor and an activated sludge process at high solids retention time. Water Res. 40, 2405–2415. Moteleb, M. A., Suidan, M. T., Kim, J. & Maloney, S. W. Pertubated loading of a formaldehyde waste in an anaerobic granular activated carbon fluidized bed reactor. Water Res. 36, 3775–3785. Nielsen, J. L. & Nielsen, P. H. Enumeration of acetateconsuming bacteria by microautoradiography under oxygen
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and nitrate respiring conditions in activated sludge. Water Res. 36, 421–428. Niemi, R. M., Heiskanen, I., Heine, R. & Rapala, J. Previously uncultured β-Proteobacteria dominate in biologically active granular activated carbon (BAC) filters. Water Res. 43, 5075–5086. Niquette, P., Prévost, M., MacLean, R. G., Thibault, D., Coallier, J., Desjardins, R. & Lafrance, P. Backwashing first-stage sand-BAC filters. Does it increase removal of biodegradable organic matter and ammonia? J. Am. Water Works Assoc. 90, 86–97. Nishijima, W., Shoto, E. & Okada, M. Improvement of biodegradation of organic substance by addition of phosphorus in biological activated carbon. Water Sci. Technol. 36 (12), 251–257. Papineau, I., Tufenkji, N. & Barbeau, B. Impact of media aging on the removal of Cryptosporidium in granular media filters. J. Environ. Eng. 139, 603–611. Quintelas, C., Fernandes, B., Castro, J., Figueiredo, H. & Tavares, T. Biosorption of Cr(VI) by a Bacillus coagulans biofilm supported on granular activated carbon (GAC). Chem. Eng. J. 136, 195–203. Satyawali, Y. & Balakrishnan, M. Effect of PAC addition on sludge properties in an MBR treating high strength wastewater. Water Res. 43, 1577–1588. Servais, P., Billen, G., Ventresque, C. & Bablon, G. P. Microbial activity in GAC filters at the Choisy-le-Roi treatment plant. J. Am. Water Works Assoc. 83, 62–68. Stoquart, C., Servais, P., Bérubé, P. & Barbeau, B. Hybrid membrane processes using activated carbon treatment for drinking water production: a review. J. Membr. Sci. 411–412, 1–12. Stoquart, C., Vázquez-Rodríguez, G. A., Servais, P. & Barbeau, B. Gamma irradiation: a method to produce an abiotic control for biological activated carbon. Environ. Technol. doi:10.1080/09593330.2013.803132. Tay, J.-H., Liu, Q.-S. & Liu, Y. The role of cellular polysaccharides in the formation and stability of aerobic granules. Lett. Appl. Microbiol. 33, 222–226. Urfer, D. & Huck, P. M. Measurement of biomass activity in drinking water biofilters using a respirometric method. Water Res. 35, 1469–1477. Velten, S., Boller, M., Köster, O., Helbing, J., Weilenmann, H. U. & Hammes, F. Development of biomass in a drinking water granular active carbon (GAC) filter. Water Res. 45, 6347–6354. Wang, J. Z., Summers, R. S. & Miltner, R. J. Biofiltration performance: part 1, relationship to biomass. J. Am. Water Works Assoc. 87, 55–63. Yener, J., Kopac, T., Dogu, G. & Dogu, T. Dynamic analysis of sorption of methylene blue dye on granular and powdered activated carbon. Chem. Eng. J. 144, 400–406.
First received 12 January 2013; accepted in revised form 1 August 2013. Available online 23 September 2013
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Genotoxicity of disinfection by-products (DBPs) upon chlorination of nine different freshwater algal species at variable reaction time Y. L. Zhang, B. P. Han, B. Yan, Q. M. Zhou and Y. Liang
ABSTRACT Nine local dominant freshwater algal species, including green algae (Chlorella sp., Chlamydomonas sp. and Scenedesmus quadricauda), diatom (Navicula pelliculosa, Nitzschia palea Grunow and Synedra sp.), blue-green algae (Microcystis sp., Chroococcus sp. and Gloeocapsa sp.) were isolated from source water reservoirs and cultivated in the laboratory. The algal biomass was chlorinated (20 C, pH 7, residual chlorine 2 mg L 1). Yields of chloroform, dichloroacetic acid, trichloroacetic W
acid, dichloroacetonitrile and trichloroacetonitrile and genotoxicity of the chlorinated solutions at eight chlorination intervals (0.5, 1, 2, 5, 10, 30, 60 and 120 min) were determined via SOSChromoTest and Comet assay. The results showed that green algae and diatom were more effective disinfection by-products (DBPs) precursors than blue-green algae. Genotoxicity was shown to be chlorination time-dependent, in agreement with our previous findings, suggesting that intermediate DBPs rather than trihalomethanes or haloacetic acids were major contributors to the genotoxicity of chlorinated solutions. Key words
| algal species, Caco-2 cells, chlorination time, Comet assay, genotoxicity, SOSChromoTest
Y. L. Zhang B. Yan Q. M. Zhou Y. Liang (corresponding author) Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen 518055, China E-mail: yliang@hkbu.edu.hk Y. L. Zhang Y. Liang Department of Environmental Pollution and Process Control, Xinjiang Institute of Ecology and Geography, Chinese Academy of Sciences, P.O. Box 9825, Beijing 100029, China; Center for Food Safety and Environmental Technology, Guangzhou Institute of Advanced Technology, Chinese Academy of Sciences, Guangzhou 511458, China; and Department of Biology, Hong Kong Baptist University, Kowloon, Hong Kong SAR, China B. P. Han Institute of Hydrobiology Jinan University, Guangzhou 510632, China Q. M. Zhou Department of Geography, Hong Kong Baptist University, Kowloon, Hong Kong SAR, China
INTRODUCTION Chlorination is widely used in water disinfection due to its
the identified chlorination DBPs seems to be a plausible
low cost and effectiveness in eliminating pathogenic micro-
bladder carcinogen (Hrudey ). Emerging DBPs such
organisms. Disinfection by-products (DBPs) are generated
as
when free chlorine reacts with natural organic matter in
derivatives are likely to be of health concern, according to
the source water. There is considerable epidemiological evi-
a recent analysis based on quantitative structure toxicity
dence for urinary bladder cancer being causally associated
relationship (Bull et al. ). These DBPs appear to be inter-
with chlorination DBPs, and that evidence for colon and
mediate DBPs during disinfection and can be further
rectal cancer is suggestive (IARC ). Currently nearly
oxidized (e.g. with prolonged chlorination), while intermedi-
700 DBPs have been reported in the literature, but none of
ate DBPs are likely to be of health concern since the
doi: 10.2166/aqua.2013.107
haloquinones,
halo-cyclopentene
and
cyclohexene
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mutagenicity of the chlorinated algal fractions (cells and
In this study, nine dominant local freshwater algal species,
proteins) reached a peak level shortly after chlorination
including green algae (chlorophyta), blue-green algae (cyano-
and then declined afterwards, different from that of chloro-
bacteria) and diatoms (bacillariophyta), were isolated in the
form (CHCl3) generation (Lui et al. , ).
source water (Hu et al. ; Liang et al. ). It was reported
In contrast with many other places, where as much as
that the DOC of surface water is about 1.69–2.18 mg L 1 in this
50% of dissolved organic carbon (DOC) is composed
region (Liang et al. ). We use a DOC concentration of
mainly of humic substances in most natural waters (Nikolaou
50 mg L 1 to quantify algal cells to standardize organic precur-
et al. ), in the Pearl River Delta region (China), the DBP
sor concentration among nine algal species, so that chlorine
precursors in some drinking water reservoirs are primarily
consumption and DBPs production could be easily compared.
from algae (Hong et al. a). During the algal blooming sea-
Changes in genotoxicity at different chlorination times were
sons, the increase in algal biomass and algal-derived organic
examined using Escherichia coli SOS-ChromoTest and Comet
matter may contribute to total organic carbon (TOC) and
assay using human Caco-2 cells. The major objectives were:
DBP formation. Algae are the major sources of dissolved
(1) to identify algal species as effective DBPs precursors in the
organic nitrogen (DON) in natural waters (Westerhoff &
source water; and (2) to identify a pattern of genotoxicity as a
Mash ). Algae cells contain a wide range of organic nitro-
function of chlorination time. We hope information from this
gen compounds, such as polysaccharides, proteins, peptides,
study could contribute to controlling DBPs precursors in the
etc. These organic compounds may contribute to DBPs for-
source water and formation of genotoxic DBPs in chlorination.
mation and particularly to prominent DBP species such as trihalomethanes (THMs) and haloacetic acids (HAAs) (Scully et al. ; Hureiki et al. ; Westerhoff & Mash
MATERIALS AND METHODS
). DON can be transformed to nitrogen-containing DBPs (N-DBPs) during chlorination or chloramination and
Algal culture
non-regulated N-DBPs are considered more toxic than the regulated THMs and HAAs (Richardson et al. ). The role of algae in DBP formation has been investigated
Nine species of algae (chlorophyta: Chlorella sp., Chlamydomonas
sp.
and
Scenedesmus
quadricauda;
cyanophyta:
in several studies (Wardlaw et al. ; Graham et al. ;
Microcystis sp., Chroococcus sp. and Gloeocapsa sp.; diatom:
Glezer et al. ; Plummer & Edzwald ; Nguyen et al.
Navicula pelliculosa, Nitzschia palea Grunow and Synedra
; Hong et al. a; Lui et al. , ). Both the
sp.) algae were obtained from the Limnology Institute of Jinan
nature of precursors and treatment conditions (e.g. pH, reac-
University, previously isolated in reservoirs at the Pearl River
tion time, temperature and relative amount of chlorine)
Delta region. Blue-green and the green alga were cultured in
determine concentration and composition of DBPs (Amy
BG11 medium (Stainer et al. ) and diatoms in diatom
et al. ), which in turn result in different toxicities in chlori-
medium (DM) in 5 L glass jars, at 25 ± 2 C under 1000 lux of
nated drinking water (Marabini et al. ; Pereira et al. ;
illumination with a 14:10 h light:dark cycle. Daily counting
Shi et al. ). Composition of algal cells plays an important
was undertaken using a light microscope and optical density
role in DBPs formation during chlorination. Generally, blue-
(OD 680 nm) was used to quantify the algal biomass. When
green algae have a higher protein content than diatoms, while
the algal growth reached log phase, the algal biomass was har-
diatoms accumulate more lipids than blue-green algae and
vested by centrifugation (3000 rpm, 10 min) and rinsed using
green algae (Hong et al. a). For algal cells, extracellular
Milli-Q water. The pellet was regarded as the algal cell fraction
organic matter and algal fractions (cells and proteins) of
and stored at 80 C, avoiding light.
W
W
different algae species were also reported to produce DBPs in different compositions (Wardlaw et al. ; Huang et al.
Chlorination
; Lui et al. ). The majority of the DBP precursors (70%) was attributable to the cellular material (Plummer &
The algal cell pellets were crushed using a liquid nitrogen
Edzwald ).
grinding method and solutions containing algal-derived
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organic materials (with starting DOC of 50 mg C L 1) were
PQ37 strain supplied by EBPI (Brampton, Ontario,
used for chlorination. Chlorination was conducted with eight
Canada), which was then modified according to Quillardet
different chlorine contact times (0.5, 1, 2, 5, 10, 30, 60 and
& Hofnung () and Mersch-Sundermann et al. ().
120 min). All samples were dissolved in phosphate buffer
Briefly, the bacteria were first incubated in growth
(pH 7, 0.2 M NaH2PO4 and 0.2 M NaOH) to maintain the
medium for 8–12 hours at 37 C. The bacterial suspension
pH. DOC was detected using a TOC analyzer (Shimadzu
was diluted using 10% DMSO in sterile 0.85% saline to
W
TOC 5000). The stock chlorine solution (NaOCl, 49.7 mg Cl2
OD 0.05–0.06 at 600 nm. Six concentration levels of posi-
mL 1) was standardized by the N,N-diethyl-p-phenylenedia-
tive controls (4 Nitro Quinoline Oxide, 4NQO) and
mine titrimetric method (APHA ). Excess chlorine was
chlorinated algal solutions were prepared respectively by
applied based on a chlorine demand test conducted before-
two-fold dilution using 10% DMSO saline. After adding
hand to ensure a substantial residual of chlorine (about 2 mg
10 μL samples into microwells, 100 μL of bacteria suspen-
1
L ) after the chlorination period. All chlorination exper-
sion were transferred into each well. The microplate was
iments were conducted at 20 C in 80 mL glass tubes with
incubated at 37 C for 2 h. Activities of β-galactosidase
glass septa in the dark. At the end of the chlorination period,
and alkaline phosphatase were then determined using 5-
samples for THM analyses were collected, head-space free, in
bromo-4-chloro-3-indolyl-β-D-galactoside (X-gal, MYM Bio-
20 mL glass vials containing Na2S2O3 quenching agent,
logical Technology Co. Ltd) and p-nitrophenyl phosphate
while samples for HAA analyses were collected in vials with
(PNPP, MYM Biological Technology Co. Ltd) disodium
NH4Cl quenching agent. Residue chlorine of samples for the
substrates, respectively. The ratio of the activities, β-galac-
toxicity test was quenched with a moderate amount of Na2SO3.
tosidase/alkaline phosphatase, divided by the values of
W
W
control samples (10% DMSO) was calculated as the inducDBPs analysis
tion factor. The induction factor increased with sample dose, and SOS inducing potency (SOSIP) was calculated
DBPs including CHCl3, dichloroacetic acid (DCAA), trichlor-
as the slope of the linear region.
oacetic acid (TCAA), dichloroacetonitrile (DCAN) and trichloroacetonitrile (TCAN) were analyzed. Briefly, CHCl3
Comet assay using Caco-2 cells
was extracted by pentane and determined according to the Standard Method (APHA ). DCAA and TCAA were extracted
Human Caco-2 cell line was obtained from the American
by methyl tert-butyl ether (MTBE) and methylated by acidic
Type Culture Collection (ATCC, Rockville, MD). The cells
methanol, and determined following USEPA (). DCAN
were cultured in Dulbecco Modified Eagle’s Medium
and TCAN were extracted by MTBE, and analyzed according
(DMEM) supplemented with 20% fetal bovine serum (FBS),
to the USEPA (). 1,2-Dibromopropane was used as the
in a humidified atmosphere of 95% air and 5% CO2 at
internal standard. The DBPs were determined by a GC-ECD
37 C. The medium was changed every 3 days and the cells
system (with a 30 m × 0.25 mm × 0.25 μm HP-5 capillary
were sub-cultured every 7 days when 95% cells confluenced.
W
column) using nitrogen as the carrier gas. The recovery rates
Oxiselect Comet Assay Kit (Cell Biolabs, Inc.) was used
for CHCl3, DCAA, TCAA, DCAN, TCAN, 1,1-DCP and 1,1,1-
for Comet assays. Procedures mainly followed the product
TCP were 97.5 ± 6.34, 101 ± 8.4, 97.3 ± 5.3, 90.7 ± 4.7,
manual with some modifications according to Fairbairn
87.7 ± 10.4, 102.7 ± 10.4 and 105.6 ± 8.2, respectively. The
et al. () and Klaude et al. (). Briefly, Caco-2 cells
detection limits for CHCl3, DCAA and TCAA were 0.00938,
were incubated in a 12-well plate at a density of 1 × 105
1
0.0105 and 0.00894 μmol L , respectively.
cells per well in 1 mL DMEM with 20% FBS. After 24 h, cells settled and formed a monolayer. Cell viability
SOS-ChromoTest
was determined via observing the color change of 3-(4,5-dimethylthiazol-2-yl)-2,5-diphenyltetrazolium
bro-
SOS-ChromoTest was initially performed without meta-
mide (MTT). Only cells with viability of more than 80%
bolic activation using an SOS-ChromoTest Kit and E. coli
were used for toxicity tests. The cells were then washed
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with phosphate-buffered saline (PBS, without Mg2þ and
centrifuged, the supernatant discarded and suspended in
Ca2þ) and treated with different samples, and cells treated
100 μL ice-cold PBS. The cells then were mixed with low
simply with DMEM medium (Milli-Q water prepared) were
melting point agarose (37 C) 1:10 briefly and spread on a
used as the control. The MEM powder was dissolved directly
slide using 75 μL mixture per well, at 4 C, avoiding light,
into the chlorinated solutions, followed by filtration through
until solidification. The cells were lysed in lysis buffer at
0.22 μm acetate cellulose membrane before incubation with
4 C for 1 h, and then in alkaline buffer for 30 min (protected
W
W
W
W
the cells. After treatment for 1 h (at 37 C, with 5% CO2), the
from
cells were collected and washed once with ice-cold PBS,
Tris-borate-EDTA (TBE) buffer twice. Electrophoresis was
Table 1
|
light),
followed
by
washing
with
ice-cold
CHCl3, DCAN and TCAN formation (mean ± SD, μmol L 1) among nine species during different chlorination time
Chlorophyta
Diatom
Cyanophyta
Time (min) CHLO
CHLA
SCEN
NAVI
NITZ
SYNE
MICR
CHRO
GLOE
CHCl3 0.5
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
1
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
2
N.D.
N.D.
17.9 ± 0.106a
16.6 ± 2.01ab
N.D.
9.49 ± 2.54c
N.D.
9.74 ± 2.34c
5
N.D. e
31.0 ± 0.991
a
36.1 ± 0.053
ab
a
36.8 ± 0.0277 6.25 ± 0. 103 c
10
8.56 ± 0.111
30
25.3 ± 0.293abc 61.8 ± 0.247ab 63.7 ± 0.100a
60
54.3 ± 15.2
120 136 ± 4.14
c
ab
99.2 ± 1.12
b
b
136 ± 1.18
29.5 ± 0.240 108 ± 0.111
a
168 ± 0.578
a
10.9 ± 1.42
e
e
32.7 ± 2.62
c
43.3 ± 0.386
11.4 ± 3.96
bc
22.8 ± 0.158abc 15.3 ± 6.37
cde
16.7 ± 0.336
d
N.D. b
9.26 ± 0.182de
18.4 ± 0.214
N.D. 10.1 ± 0.278
e
a
16.1 ± 0.101d
38.7 ± 1.74
44.9 ± 8.45abc 27.8 ± 0.207abc 9.99 ± 0.100c 41.2 ± 29.2bc ab
38.8 ± 1.48
c
106 ± 5.12
54.9 ± 11.4
d
N.D.
88.3 ± 6.48 f
13.8 ± 0.656
bc
c
17.5 ± 0.378
c
29.2 ± 0.272
g
23.5 ± 7.82abc
c
30.1 ± 1.64c
45.8 ± 0.00
e
77.8 ± 0.0404 31.3 ± 3.18g
DCAN 0.5
49,197 ± 244a c
24.8 ± 6.34bc c
270 ± 72.9bc
N.D.
N.D.
472 ± 51.0a
N.D.
14.0 ± 0.962c N.D.
N.D.
N.D.
199 ± 27.2b
10.3 ± 6.23c
N.D.
b
c
9.64 ± 2.92
N.D.
11.4 ± 0.489b
N.D.
15.5 ± 0.883c
N.D.
1
53.2 ± 0.788
2
4,330 ± 205
a
28.0 ± 6.87
52.7 ± 26.4
13.4 ± 0.236
10.6 ± 2.27
48.0 ± 5.56
111 ± 94.0
5
86.2 ± 3.14ab
188 ± 161ab
130 ± 46.3ab
34.4 ± 10.0ab
N.D.
9.24 ± 0.552b
272 ± 33.0a
10
78.6 ± 0.126b
155 ± 7.63a
23.7 ± 6.43c
49.0 ± 7.72bc
N.D.
N.D.
78.4 ± 19.5b
29.2 ± 3.90
b
95.8 ± 4.45
b
15.5 ± 2.76
c
1,730 ± 71.4
120 17.7 ± 1.21c
21.0 ± 3.39c
30 60
b
bc
247 ± 12.6
a
b
63.4 ± 9.65
729 ± 469
a
b
cd
b
14.8 ± 11.7
d
9.25 ± 0.788
19.9 ± 1.56
c
60.2 ± 1.33a
N.D.
N.D.
N.D.
21.4 ± 2.21
d
24.8 ± 0.835
40.3 ± 4.18b
b
43.0 ± 16.3 c
c
d
18.4 ± 5.28
c
N.D.
d
19.0 ± 3.07d
c
13.2 ± 1.58
31.4 ± 14.3
12.8 ± 5.12
15.3 ± 3.94c
N.D.
35.1 ± 1.50b
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
TCAN 0.5
2,690 ± 152a
28.9 ± 0.693b 68.1 ± 19.7b
b
b
b
b
1
32.1 ± 4.51
51.5 ± 1.24
84.0 ± 12.0
N.D.
94.2 ± 19.7
N.D.
963 ± 233a
N.D.
N.D.
2
2,380 ± 113b
140 ± 6.96d
3,260 ± 29.7a
N.D.
797 ± 40.1c
75.3 ± 21.0d
17.6 ± 4.31d
N.D.
N.D.
5
47.4 ± 1.73e
300 ± 0.910b
137 ± 2.84c
N.D.
465 ± 0.780a
11.5 ± 0.633f
128 ± 9.34cd
N.D.
c
b
c
b
c
10
43.2 ± 0.0693
215 ± 2.64
35.4 ± 1.26
N.D.
223 ± 37.7
30
50.1 ± 1.18cd
173 ± 37.0b
17.2 ± 0.568d
9.72 ± 2.81d
1,440 ± 23.9a 36.2 ± 0.711cd
36.8 ± 8.54cd 230 ± 8.10b
92.5 ± 27.6c
60
N.D.
88.4 ± 4.36bc
323 ± 63.8a
12.7 ± 4.89c
168 ± 19.0b
20.0 ± 0.793c
45.7 ± 14.7c
176 ± 22.2b
10.6 ± 1.43c
N.D.
22.5 ± 4.42
77.8 ± 2.46
N.D.
46.0 ± 5.42
24.1 ± 12.2
N.D.
120 9.75 ± 0.667
d
55.5 ± 2.11
ab
d
a
N.D.
50.0 ± 2.31
109 ± 13.4d a
bc
542 ± 29.9
cd
N.D.
Means containing the same letter were not significantly different (p > 0.05), according to multiple-comparison of means by one-way ANOVA. Detection limits of CHCl3, DCAN and TCAN were 9.38, 9.00 and 9.42 pmol L 1 respectively. N.D.: not detectable; CHLO: Chlorella sp.; CHLA: Chlamydomonas sp.; SCEN: Scenedesmus quadricauda; NAVI: Navicula pelliculosa; NITZ: Nitzschia palea Grunow; SYNE: Synedra sp.; MICR: Microcystis sp.; CHRO: Chroococcus sp.; GLOE: Gloeocapsa sp.
16
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performed at 4 C, 1 V cm 1, for 15 min in TBE. Afterwards,
SPSS (Statistic Package for Social Science) software pro-
the slides were neutralized using pre-chilled DI water,
gram for Microsoft Windows (Version 16.0) (SPSS Inc.).
W
dehydrated with 70% ethanol, and stained using vista green DNA dye for 15 min. The cells were measured for their comet tail moment (TM) using a fluorescence microscope with a CCD camera, to indicate DNA damage in the treated cells. About 50 cells per treatment were randomly measured, and the same level of treatment was conducted in three different generations of cells. Values of average TM were calculated from 50 cells exposed to the same level of treatment.
RESULTS AND DISCUSSION DBPs yields among different algal species In general, algal organic matter upon chlorination was more effective in generating CHCl3 than the other measured DBPs (Tables 1 and 2). In particular, among different species, green algae were shown to form more CHCl3
Data analysis
upon chlorination than the other algal species. At 120 min chlorination time, the highest yield of CHCl3 was
One-way analysis of variance (ANOVA) and independent t-
observed to be formed from Scenedesmus quadricauda
test were used to compare the means analyzed using the
(168 μmol L 1), 5.75 times of that from Microcystis sp.
Table 2
|
DCAA and TCAA formation (mean ± SD, μmol L 1) among nine species during different chlorination time Chlorophyta
Time (min)
Diatom
CHLO
CHLA
0.5
N.D.
1
N.D.
2 5
SCEN
Cyanophyta
NAVI
NITZ
SYNE
MICR
CHRO
GLOE
N.D. N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
N.D. N.D.
N.D.
N.D.
N.D.
60.2 ± 16.0
N.D.
N.D.
13.6 ± 3.61a
N.D. N.D.
13.8 ± 5.12a
19.5 ± 0.413a
15.3 ± 1.36a
N.D.
N.D.
11.6 ± 0.867a
12.5 ± 1.18c
N.D. N.D.
46.2 ± 4.07b
N.D.
87.0 ± 13.2a
21.6 ± 3.41c
28.5 ± 0.335bc
DCAA
ab
c
10
113 ± 1.40
30
18.5 ± 0.447b N.D. 33.6 ± 1.45b a
N.D. 17.2 ± 2.39
c
c
31.7 ± 7.55 N.D.
a
32.0 ± 4.39
N.D.
105 ± 9.57a
22.1 ± 2.27b
a
a
133 ± 11.4
N.D. N.D.
35.3 ± 0.0576b
N.D. a
84.2 ± 1.24b
19.0 ± 0.369
31.1 ± 11.1
26.1 ± 1.47a
18.3 ± 3.41bc N.D.
41.9 ± 3.82b
182 ± 12.5a
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
14.3 ± 1.20
a
35.6 ± 0.956bc
a
60
19.4 ± 0.440
N.D. N.D.
16.4 ± 0.972
16.4 ± 3.58
120
26.2 ± 2.06bc
N.D. 12.5 ± 3.29c
18.9 ± 5.53bc
0.5
N.D.
N.D. N.D.
1
10.8 ± 0.246
N.D. N.D.
2
N.D.
N.D. N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
12.4 ± 3.80
5
361 ± 50.1a
N.D. N.D.
13.9 ± 2.93b
N.D.
N.D.
10.4 ± 1.22b
46.2 ± 8.55b
N.D.
10
N.D.
N.D. 448 ± 84.2a
N.D.
N.D.
N.D.
9.06 ± 0.538b 16.7 ± 0.661b
N.D.
TCAA
a
a
30
N.D.
N.D. 19.3 ± 4.41
N.D.
12.9 ± 2.75
N.D.
N.D.
N.D.
N.D.
60
N.D.
N.D. N.D.
11.4 ± 4.04a
N.D.
N.D.
N.D.
N.D.
11.1 ± 1.46a
120
N.D.
N.D. 18.8 ± 0.369 N.D.
N.D.
N.D.
N.D.
N.D.
N.D.
Means containing the same letter were not significantly different (p > 0.05), according to multiple-comparison of means by one-way ANOVA. Detection limits of DCAA and TCAA were 10.5 and 8.94 pmol L 1 respectively. N.D.: not detectable; CHLO: Chlorella sp.; CHLA: Chlamydomonas sp.; SCEN: Scenedesmus quadricauda; NAVI: Navicula pelliculosa; NITZ: Nitzschia palea Grunow; SYNE: Synedra sp.; MICR: Microcystis sp.; CHRO: Chroococcus sp.; GLOE: Gloeocapsa sp.
17
Figure 1
Y. L. Zhang et al.
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Genotoxicity of chlorinated algal organic materials
Journal of Water Supply: Research and Technology—AQUA
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Time-dependent changes in genotoxicity of chlorinated algae using SOS-test: (a) SOSIP change among green algae; (b) SOSIP among diatom; (c) SOSIP among blue-green algae. CHLO: Chlorella sp.; CHLA: Chlamydomonas sp.; SCEN: Scenedesmus quadricauda; NAVI: Navicula pelliculosa; NITZ: Nitzschia palea Grunow; SYNE: Synedra sp.; MICR: Microcystis sp.; CHRO: Chroococcus sp.; GLOE: Gloeocapsa sp.
(29.2 μmol L 1). Meanwhile, it is also observed that different
et al. ). Particularly, DCAN formation was the highest
algal species in the same group had significant differences in
(0.492 μmol L 1) at 0.5 min chlorination of Chlorella sp.,
CHCl3 formation. For example, at 120 min, Nitzschia palea
and the highest TCAN (3.26 μmol L 1) was observed at
CHCl3
2 min chlorination of Scenedesmus quadricauda. The data
(106 μmol L 1) than the other two diatoms (Navicula pelli-
were consistent with a previous study by Nguyen et al.
Grunow
(diatom)
produced 1
culosa 43.3 μmol L
relatively
more
1
and Synedra sp. 54.9 μmol L );
() that green algae were more productive in generating
Chroococcus sp. (blue-green algae) produced 77.8 μmol L 1
CHCl3 than blue-green algae and diatoms (Nguyen et al.
CHCl3, twice higher than the other two blue-green algal
). However, in our previous report of CHCl3 formation
species (Microcystis sp. 29.2 μmol L 1 and Gloeocapsa
after 4 d chlorination, the diatom was shown to be the most
sp. 31.3 μmol L 1). The comparison among different algal
effective precursor (Hong et al. b). Obviously chlori-
species was similar in DCAN and TCAN formation
nation time is another key factor in determining CHCl3
(Table 1), as these two DBPs are generally regarded as inter-
generation. On the other hand, Chroococcus sp. (blue-
mediate chlorination products in the process of CHCl3
green algae) formed the highest concentration of DCAA
formation (Peters et al. ; Nikolaou et al. ; Reckhow
(peak level for 0.182 μmol L 1 at 120 min chlorination)
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among all the algal species, while minor amounts of TCAA
genotoxicity and any of the DBP level was not significant
were generated (Table 2). Whether this is due to generally
and therefore the specific responsible DBPs were not ident-
higher protein in blue-green algae (Hong et al. b)
ified. Chlorination time is determined by raw water quality
requires investigation in the future.
in the water treatment, particularly microbiological quality, while short chlorination time does not always mean less DBPs formation and the associated genotoxicity. Therefore,
Genotoxicity
a sound control of chlorination time means a good A preliminary study was conducted using unchlorinated algal cells at 50 mg L
1
TOC, and no genotoxicity was
reduction in both pathogens and genotoxic DBPs in water treatment.
detected. All chlorinated solutions showed genotoxicity (Figure 1), and chlorination time appeared to be a critical contributor. Most solutions showed that peak levels of genotoxicity
were
reached
before
30 min
(except
CONCLUSIONS
for
Gloeocapsa sp. at 60 min) and then reduced when chlori-
DBPs formation was different among nine different species
nation time was prolonged. A similar pattern was observed
of algal cells during chlorination. CHCl3 formation
previously (Lui et al. , ), suggesting that intermediate
increased as chlorination time increased while the other
by-products generated within a very short reaction time were
DBPs (DCAA, TCAA, DCAN and TCAN) showed a peak
responsible for the fluctuation. A general pattern is observed
level before 120 min. Green algae generally formed a
that chlorinated green algal solutions, containing higher
higher level of CHCl3. DCAN and TCAN also reached
levels of CHCl3, DCAN and TCAN (Table 1 and Figures 1
higher levels within 120 min. Blue-green algae produced
and 2), were more genotoxic. Both chlorinated Synedra sp.
relatively lower DBPs and also showed lower genotoxicity
(diatom) and Gloeocapsa sp. (blue-green algae) formed rela-
than green algae and diatom. DBPs formation and toxicity
tively less DBPs (especially for DCAN and TCAN) during
differs among different algal groups, and also different
chlorination (Table 1) and also showed relatively lower gen-
algal species in the same group.
otoxicity (Figure 1). However, the link between the
ACKNOWLEDGEMENTS This research was funded by the International Science & Technology
Cooperation
Program
of
China
(2010DFA92720-24). This study was also supported by the Faculty Research Grant (FRG2/11-12/037, Faculty of Science of Hong Kong Baptist University) and ‘One Hundred Talents’ (Chinese Academy of Science, China) awarded to Yan Liang.
REFERENCES
Figure 2
|
Average tail moment of Caco-2 cells by the Comet assay, comparing among different algal species. Means containing the same letter were not significantly different (p > 0.05), according to multiple-comparison of means by one-way ANOVA. CHLO: Chlorella sp.; CHLA: Chlamydomonas sp.; SCEN: Scenedesmus quadricauda; NAVI: Navicula pelliculosa; NITZ: Nitzschia palea Grunow; SYNE: Synedra sp.; MICR: Microcystis sp.; CHRO: Chroococcus sp.; GLOE: Gloeocapsa sp.
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US Environmental Protection Agency (USEPA) Method 552.3: Determination of Haloacetic Acids and Dalapon in Drinking Water by Liquideliquid Microextraction, Derivatization, and Gas Chromatography with Electron Capture Detection. EPA 815-B-03-002. Revision 1.0. US Environmental Protection Agency, Washington, DC. US Environmental Protection Agency (USEPA) Method 551.1: Determination of Chlorination Disinfection Byproducts, Chlorinated Solvents, and Halogenated
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First received 3 June 2013; accepted in revised form 22 August 2013. Available online 15 October 2013
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Relationships between trihalomethanes, haloacetic acids, and haloacetonitriles formed by the chlorination of raw, treated, and fractionated surface waters Paolo Roccaro, Federico G. A. Vagliasindi and Gregory V. Korshin
ABSTRACT This study examined effects of coagulation and fractionation of natural organic matter on the distribution of trihalomethanes (THM), haloacetic acids (HAA), and haloacetonitriles (HAN) formed in chlorinated water. The precursors of HAA and THM were determined to be associated primarily with the hydrophobic fraction although the hydrophilic fraction is important as well. On the other hand, the precursors of HAN are overwhelmingly hydrophilic with only a negligible contribution of the hydrophobic and transphilic fractions. Higher percentages of HAN were found in the treated waters compared with raw waters, collected from three different full scale water treatment plants. Very strong correlations were found between THM, HAA, and HAN concentrations. Two main correlations between THM and HAN were observed. One was applicable to all raw waters regardless of their fractionation and provenance, while the other was formed by the treated waters, again regardless of
Paolo Roccaro (corresponding author) Federico G. A. Vagliasindi Department of Civil and Environmental Engineering, University of Catania, Viale A. Doria, 6, 95125, Catania, Italy E-mail: proccaro@dica.unict.it Gregory V. Korshin Department of Civil and Environmental Engineering, University of Washington, Seattle, WA 98195-2700, USA
their source and fractionation. This result emphasizes that a significant removal of THM and HAA precursors can be achieved via coagulation but it results in a negligible removal of HAN precursors. As a consequence, some changes in treatment trains or operating conditions may need to be considered to minimize the formation of HAN. Key words
| coagulation, disinfection by-products, drinking water, fractionation, hydrophilic natural organic matter
INTRODUCTION Chlorination of drinking water in public facilities was one of
; Krasner et al. ), but other water quality parameters
the most important public health measures during the twen-
(e.g., pH, temperature, bromide, and iodide) can impact
tieth century because it reduced the transmission of deadly
the concentration and speciation of DBP (Obolensky &
waterborne diseases such as typhoid and cholera. Apart
Singer ). Trihalomethanes (THM) and haloacetic acids
from the limited disinfection efficiency against some chlor-
(HAA) are generally present at the highest levels (from a
ine-resistant pathogens, the main drawback of chlorination
few to hundred ppb) in chlorinated drinking water. Among
is the formation of harmful disinfection by-products (DBP)
known but unregulated DBP, several species have been
that result from reactions between chlorine and both natural
found in drinking waters at much lower concentrations
organic matter (NOM) present in all source water or effluent
than those of THM and HAA but their potential toxicity is
organic matter (EfOM) occurring in wastewater impacted
higher (Roccaro et al. ; Richardson et al. ). Recent
water bodies (Krasner et al. ; Sedlak & von Gunten
studies (Muellner et al. ; Richardson et al. ;
).
Plewa et al. ) have determined that the nitrogenous
The content and reactivity of NOM and EfOM plays a
DBP (N-DBP) are much more toxic than carbonaceous
major role in the formation of DBP (Leenheer & Croue
DBP (C-DBP). Haloacetonitriles (HAN) are a class of
doi: 10.2166/aqua.2013.043
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nitrogen-containing DBP which are ubiquitous in chlori-
mg 1 m 1 for MS, MF, DS, and DF samples, respectively.
nated waters (Richardson et al. ) and due to their high
The bromide level in Ancipa and Potomac water was
cytotoxicity and genotoxicity require more consideration
about 0.05 mg/L.
(Muellner et al. ).
All samples were filtered through a 0.45 mm nylon
Although several studies have been carried out to exam-
membrane filter (Polycap AS Capsule Filter) and stored at
ine the relationships and relative distributions between DBP
4 C. All chemicals were ACS reagent grade or better. Sol-
W
species (Liang & Singer ; Serodes et al. ; Malliarou
vents used in extractions were high-purity grade. Reagent
et al. ), these relationships have not been fully investi-
water was obtained from a Millipore Super-Q Plus water
gated for nitrogenous DBP such as HAN. Accordingly, the
system. Chlorine stock solution was prepared by dilution
objective of this study was to examine the yields and specia-
of a reagent-grade sodium hypochlorite solution (5% avail-
tion of regulated DBP (THM and HAA) and emerging DBP
able chlorine) with Milli-Q water. Amberlite XAD-8 (now
(HAN) in chlorinated raw, treated, and fractionated surface
called Supelite DAX-8, Supelco #20278) and Amberlite
waters at varying reaction conditions.
XAD-4 (Supelco #20276) resins were used for all fractionation procedures.
MATERIALS AND METHODS
Experimental methods
Water sources and materials
NOM fractionation was carried out using the simplified NOM fractionation scheme that utilized small (8 mL) resin
Experiments were conducted using water samples from the
volumes packed into a 30 cm × 1.0 cm (24 mL) glass
inlet and outlet of a water treatment plant (WTP) that treats
column. XAD-8 and XAD-4 resins were used for all fraction-
the water from Ancipa reservoir (Sicily, Italy) and water
ation
samples from the Potomac River (Washington, DC) and from
hydrophobic (HPO), transphilic (THP), and hydrophilic
two WTPs (McMillan and Dalecarlia) that utilize its water.
(HPI) fractions, following published methods (Leenheer &
The dissolved organic carbon (DOC) concentration of 1
in order to
separate NOM
into
Croue ; Roccaro & Vagliasindi ). Chlorination experiments were conducted in the dark at
the Ancipa Inlet (influent of the WTP) sample was 2.9 mg/ 1
procedures,
W
(SUVA: specific ultraviolet
20 C at chlorine doses between 1.5 and 2.0 mg of chlorine
absorption). On the other hand, the DOC in Ancipa Outlet
per mg of DOC and varying reaction time (10 min to 3
(effluent of the WTP) sample was 2.0 mg/L, SUVA254 was
days). The water samples were chlorinated with sodium
L, SUVA254 was 2.8 L mg
1
m
m . Both Ancipa Inlet and Outlet were also
hypochlorite at pH 7.0 in the presence of 0.03 mol L 1 of
fractionated and the effluents from the XAD-8 (namely
phosphate buffer. In each case the chlorinated samples col-
‘Ancipa Inlet XAD-8 effluent’ and ‘Ancipa Outlet XAD-8
lected were analyzed only if chlorine residual was found.
effluent’) and XAD-4 (namely ‘Ancipa Inlet XAD-4 effluent’
Sodium sulfite or ammonium chloride was used to quench
and ‘Ancipa Outlet XAD-4 effluent’) bench scale columns
the residual chlorine. Chlorinated samples were refrigerated
were used for chlorination as well as the unfractionated
at 4 C for no more than 10 days before being analyzed for
samples. The DOC of the Potomac water sample (Potomac
DBP concentrations.
1.8 L mg
1
W
Inlet) was 2.7 mg/L and SUVA254 was 2.4 L mg 1 m 1. At the Potomac WTPs, samples of effluents from the sedimen-
Analytical methods
tation tanks (denoted as ‘Potomac MS’ and ‘Potomac DS’ for McMillan and Dalecarlia, respectively) and from filters
DOC was analyzed using an O.I. Analytical 1010 or a
(denoted as ‘Potomac MF’ and ‘Potomac DF’ for McMillan
Shimadzu VCSH organic carbon analyzer. UV absorbance
and Dalecarlia plants) were taken. DOC values were 1.6,
was analyzed using a 5 cm quartz cell on a Perkin-Elmer
1.7, 2.0, and 2.0 mg/L for MS, MF, DS, and DF samples,
Lamda 18 UV/Vis Spectrophotometer at λ ¼ 200–600 nm.
respectively. SUVA254 values were 1.7, 1.3, 1.8, and 1.5 L
All spectra were normalized to a 1 cm cell length.
23
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Concentrations of THM, other volatile and semi-volatile
was 57, 65, 45 and 52% at Potomac MS, MF, DS, and DF,
DBP (including HAN) and HAA were determined using
respectively.
standard analytical procedures (EPA methods 551.1 and
Coagulation also resulted in consistent changes of rela-
552.2) and a Perkin-Elmer AutoSystem gas chromatograph
tive contributions of the three different classes of DBP
equipped with an electron capture detector. Other aspects
investigated, namely total HAA (THAA, sum of the nine
of these analyses are described in previous publications
chloro- and bromo-substituted HAAs), total THM (TTHM,
(Korshin et al. ; Roccaro et al. ).
sum of the four chloro- and bromo-substituted THM), and total HAN (THAN, sum of dichloroacetonitrile, bromochloroacetonitrile, dibromoacetonitrile and trichlor-
RESULTS AND DISCUSSION
oacetonitrile)
as
shown
in
Figure
1.
Indeed,
the
contribution of THAA decreased after the treatment of PotoImpact of coagulation on the removal of organic
mac water, while TTHM increased (Figure 1). The changes
precursors in the formation THM, HAA, and HAN
in the contributions of THAA and TTHM after the treatment at Ancipa WTP were almost negligible. On the other hand, a
Coagulation followed by clarification and/or filtration is the
significant increase in the contribution of THAN was
standard process used to remove turbidity and NOM from
observed for all the coagulated waters, as shown in Figure 1.
surface waters. However, the removal of NOM by coagu-
These results agree with the data of previous studies
lation is usually limited to about 30–50%, except for water
which showed that the aromatic and high molecular
with a high content of humic material which can result in
weight fraction NOM removed by coagulation contains the
removal higher than 70% (Edzwald ). Coagulation is
main precursors for HAA and some precursors for THM
more efficient for the removal of the most hydrophobic
(Liang & Singer ). However, other research suggested
and high molecular weight fraction of NOM (Chow et al.
that low-MW, non-humic NOM contributes more promi-
, ; Kim & Yu ; Matilainen et al. ). In this
nently in HAA formation (Siddiqui et al. ; Kim & Yu
study, the removal of NOM at the Ancipa WTP was 30%
). The higher relative contribution of THAN in the coa-
as DOC and 56% as A254. The DOC removal for Potomac
gulated waters observed in this study is likely to be
MS and MF was 39 and 35% as DOC, respectively, and
associated with the higher hydrophilic content in coagulated
24% for both Potomac DS and DF. The removal of A254
NOM. This finding corroborates some recent studies which
Figure 1
|
Speciation of THAA, TTHM, and THAN in chlorinated raw and treated Ancipa and Potomac waters at reaction time of 24 hours. Chlorine doses from 1.5 to 2.0 mg Cl2 per mg DOC.
24
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reported moderate removal of nitrogenous DBP (N-DBP)
NOM by coagulation plays a major role in the speciation
precursors by coagulation and higher N-DBP formation
of the investigated DBP.
in chlorinated hydrophilic fractions which are rich in nitrogen (Dotson et al. ; Bond et al. ; Shah &
Contribution of hydrophobic, transphilic, and
Mitch ).
hydrophilic fractions of NOM to the formation of THM,
It is noteworthy that the treated water contains a higher
HAA, and HAN by chlorination
bromide to DOC ratio because of the negligible removal of bromide by coagulation. Therefore, the higher contribution
In order to assess the relative contributions of NOM frac-
of a specific class of DBP in the treated water (Figure 1)
tions with different polarities in DBP formation and
may be ascribed to the higher bromide to DOC ratio. For
speciation, four rounds of NOM fractionation of Ancipa
instance, Table 1 shows the percentage distribution of
Inlet and Outlet water were carried out. These contributions
THM species for the chlorinated Ancipa and Potomac
were calculated by differences of values obtained by the
water at 24 hours of reaction time. The speciation of
chlorination of unfractionated and fractionated (XAD-8
THM, HAA, and HAN is also affected by the reaction
effluent or XAD-4 effluent) samples. In accord with prior
time, but as reported in prior research carried out on the
studies (Liang & Singer ; Hua & Reckhow ), both
Ancipa water (Roccaro et al. , ), there is a small
hydrophobic and hydrophilic fractions of Ancipa NOM
decrease of the bromine substitution in THM, HAA, and
were found to play an important role in the production of
HAN with the extent of the reaction. Overall, considering
DBP. The contributions of NOM fractions to TTHM,
the moderate level of bromide in Ancipa and Potomac
THAA, and THAN yields in Ancipa Inlet and Outlet
water, the chlorine dose and the resulting change in the spe-
waters varied with the reaction time, as shown in Figures 2
ciation of THM (Table 1), the impact of bromide in total
and 3 for experiments carried out with 1.5 mg of chlorine
THM, HAA and HAN formation is limited according to
per mg of DOC. As expected, higher reaction times were
prior research (Cowman & Singer ; Chang et al. )
associated with higher DBP yields, except for the formation
and the removal of the more aromatic and hydrophobic
of THAN by the chlorination of the THP fraction of Ancipa Inlet water (Figure 2) and for THAN formed by the chlorination of HPO and TPI fractions of Ancipa Outlet water
Table 1
|
Speciation of THM in chlorinated raw and treated Ancipa and Potomac waters at
(Figure 3). The latter result is probably due to a low
reaction time of 24 hours. Chlorine doses from 1.5 to 2.0 mg Cl2 per mg DOC
reactivity of THP and HPO fractions in HAN formation.
CHClBr2, %
CHBr3, %
The contributions of the HPI fraction to TTHM yields for
Water
CHCl3, %
CHCl2Br, %
Ancipa Inlet
83
16
1
0
Ancipa Inlet XAD-8 effluent
75
23
2
0
Ancipa Inlet XAD-4 effluent
63
31
6
0
Ancipa Outlet
71
26
4
0
Singer ), generating a large amount of TTHM and of
Ancipa Outlet XAD-8 effluent
67
27
6
0
THAA, as shown in Figure 2. A negligible contribution of
Ancipa Outlet XAD-4 effluent
59
31
10
1
Potomac Inlet
74
22
3
1
Potomac MS
68
26
6
0
Potomac MF
68
25
6
1
Potomac DS
74
22
3
1
Potomac DF
74
21
3
2
chlorinated Ancipa Inlet waters was somewhat higher than those of the HPO and THP fractions, as shown in Figure 2. In particular, the contribution of the HPI fraction increases with increasing reaction time possibly because the HPO and THP fractions react faster with chlorine (Liang &
the HPO fraction to TTHM yields was observed for chlorinated Ancipa Outlet water (Figure 3). This was apparently caused by a significant removal of the HPO fraction at Ancipa WTP. This point is confirmed by the fractionation data showing that the removal of the HPO, THP, and HPI fractions (quantified by their A254 values) at Ancipa WTP was 63, 48 and 49%, respectively. At reaction times higher than 4 hours, the NOM fraction contribution to TTHM
25
Figure 2
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Relationships between DBP formed in chlorinated waters
Journal of Water Supply: Research and Technologyâ&#x20AC;&#x201D;AQUA
Yields of THAA, TTHM, and THAN in chlorinated fractions of Ancipa raw water at varying reaction times. Chlorine dose of 1.5 mg Cl2 per mg DOC.
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26
Figure 3
P. Roccaro et al.
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Journal of Water Supply: Research and Technologyâ&#x20AC;&#x201D;AQUA
Yields of THAA, TTHM, and THAN in chlorinated fractions of Ancipa treated water at varying reaction times and chlorine dose of 1.5 mg Cl2 per mg DOC.
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27
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yields was in the order HPI > >THP ¼ HPO for Ancipa Inlet
results in the preferential removal of HAA and some THM
water and HPI > THP > >HPO for Ancipa Outlet water.
precursors (Figure 1), in accord with Liang & Singer
On the other hand, all the NOM fractions contributed
(). In contrast with this result, the hydrophilic HAN pre-
extensively to THAA yields (Figure 2), with especially pro-
cursors escape the coagulation process resulting in higher
minent contributions of both THP and HPI fractions in
relative yields (in μg per mg DOC) of THAN in coagulated
Ancipa Outlet water. These results further support the
waters, as shown in Figure 1. Furthermore, as shown in
point that the HPO fraction plays an important role in
Figure 4, the more hydrophilic NOM fractions of both
TTHM and THAA formation but the HPI fraction also con-
Ancipa Inlet and Outlet waters produced relatively lower
tains important precursors for TTHM (Liang & Singer ;
percentages of THAA and higher percentages of TTHM
Zhao et al. ) and for THAA formation (Kim & Yu ).
and THAN.
Contributions of the examined NOM fractions in THAN yields were different, with the HPI fraction being the domi-
Relationships between trihalomethanes, HAA,
nant part of NOM contributing to THAN (Figures 2 and 3).
and haloacetonitriles
In fact, relative THAN yields increased after coagulation confirming that the HPI fraction contains the major precur-
Very strong correlations were found to exist between
sors for THAN and that coagulation does not remove this
TTHM, THAA, and THAN (Figures 5 and 6). However,
fraction.
while correlations between TTHM and THAA were not sig-
Similarly to the effect of coagulation on the bromide to
nificantly affected by the alterations of NOM properties
DOC ratio, also the fractionation of NOM used in this study
caused by the treatment and/or fractionation, different pat-
increases the bromide to DOC ratio of the resulting sol-
terns were observed in the relationship between TTHM
utions and therefore the speciation of THM, HAA, and
and THAN for raw and treated samples. Two main types
THAN, as shown in Table 1 for THM, but the impact of bro-
of the observed correlations could be distinguished. One of
mide in total THM, HAA, and HAN formation is limited
them was applicable to dataset generated for the raw
according to prior research (Cowman & Singer ;
waters regardless of their fractionation and provenance
Chang et al. ).
while the other corresponded to the combined treated
Overall, the data show that coagulation removes mostly
water data, irrespective of the type of water source and frac-
the more aromatic and hydrophobic fractions of NOM. This
tionation (Figure 6). The negligible impact of fractionation
Figure 4
|
Speciation of THAA, TTHM, and THAN in chlorinated raw, treated, and fractionated Ancipa water at reaction time of 24 hours and chlorine doses from 1.5 to 2.0 mg Cl2 per mg DOC.
28
Figure 5
P. Roccaro et al.
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Correlations between concentrations of THAA and TTHM in Ancipa (raw, treated, and fractionated) and Potomac (raw and treated) waters at varying chlorination conditions (reaction time from 10 min to 3 days and chlorine doses from 0.75 to 2.0 mg Cl2 per mg DOC).
Figure 6
|
Correlations between concentrations of THAN and TTHM for Ancipa (raw, treated, and fractionated) and Potomac (raw and treated) waters at varying chlorination conditions (reaction time from 10 min to 3 days and chlorine doses from 0.75 to 2.0 mg Cl2 per mg DOC).
on these correlations emphasizes that some of the THAA
It should be recognized that the observed correlations
and TTHM precursors are hydrophilic while almost all
may not be uniformly applicable to all distribution
HAN precursors are hydrophilic and therefore their
systems because some DBP, for instance selected HAA
removal is limited.
species, may undergo decay in them (Tung & Xie ;
29
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Zhang et al. ), but this issue was not examined in this
paper do not necessarily reflect those of the funding
study.
agencies.
REFERENCES
CONCLUSIONS Results obtained in this study indicate that TTHM measurements could be used as a DBP surrogate to estimate the concentrations of the unregulated THAN whose presence in drinking water may prove to be of public health concern. The main precursors for HAA and THM were found to be associated with the hydrophobic
and
transphilic
NOM
fractions
with
the
hydrophilic fraction playing a smaller but important role. In contrast, HAN precursors were determined to be strongly associated with the hydrophilic NOM fraction, with negligible contribution of the HPO and THP fractions. The data show that because conventional full scale coagulation processes tend to preferentially remove THM and HAA precursors but not those of HAN, this results in higher relative contributions of HAN in the sum of THM, HAA, and HAN species formed in treated water. The toxicity of nitrogenous DBP, including HANs, and the relative persistence of their precursors in conventionally treated water may require that alternative advanced water treatment processes and/or operating conditions be considered to control the levels of these N-DBP in drinking water.
ACKNOWLEDGMENTS This study was partially supported by the United States EPA/Cadmus (grant 069-UW-1) and the Italian Ministry of Instruction, University, and Research (MIUR), through the program Research Projects of National Interest ‘Control and monitoring of drinking water quality’ and ‘Reuse of Wastewater in Agriculture: Emerging Pollutants and Operational Problems’. Paolo Roccaro acknowledges the US-Italy Fulbright Commission for supporting his research in the US through the ‘Fulbright Scholar Program Advanced Research and University Lecturing Awards in the United States’. Views expressed in this
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trihalomethanes in drinking water. Environ. Sci. Technol. 37 (13), 2920–2928. Malliarou, E., Collins, C., Graham, N. & Nieuwenhuijsen, M. J. Haloacetic acids in drinking water in the United Kingdom. Water Res. 39 (12), 2722–2730. Matilainen, A., Lindqvist, N. & Tuhkanen, T. Comparison of the efficiency of aluminium and ferric sulphate in the removal of natural organic matter during drinking water treatment process. Environ. Technol. 26 (8), 867–875. Muellner, M. G., Wagner, E. D., Mccalla, K., Richardson, S. D., Woo, Y.-T. & Plewa, M. J. Haloacetonitriles vs. regulated haloacetic acids: are nitrogen-containing DBP more toxic? Environ. Sci. Technol. 41 (2), 645–651. Obolensky, A. & Singer, P. C. Development and interpretation of disinfection byproduct formation models using the information collection rule database. Environ. Sci. Technol. 42 (15), 5654–5660. Plewa, M. J., Wagner, E. D., Muellnerm, M. G., Hsu, K. & Richardson, S. D. Comparative mammalian cell toxicity of N-DBP and C-DBP. ACS Symposium Series 995. In: Occurrence, Formation, Health Effects and Control of Disinfection By-products in Drinking Water (T. Karanfil, S. W. Krasner, P. Westerhoff & Y. Xie, eds). American Chemical Society, Washington, DC, pp. 36–50. Richardson, S. D., Plewa, M. J., Wagner, E. D., Schoeny, R. & DeMarini, D. M. Occurrence, genotoxicity, and carcinogenicity of regulated and emerging disinfection by-products in drinking water: a review and roadmap for research. Mutat. Res. 636 (1–3), 178–242. Roccaro, P. & Vagliasindi, F. G. A. Differential versus absolute UV absorbance approaches in studying NOM reactivity in DBP formation: comparison and applicability. Water Res. 43 (3), 744–750. Roccaro, P., Mancini, G. & Vagliasindi, F. G. A. Water intended for human consumptions – Part I: compliance with European water quality standards. Desalination 176 (1–3), 1–11. Roccaro, P., Chang, H.-S., Vagliasindi, F. G. A. & Korshin, G. V. Differential absorbance study of effects of temperature
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on chlorine consumption and formation of disinfection by-products in chlorinated water. Water Res. 42 (8–9), 1879–1888. Roccaro, P., Vagliasindi, F. G. A. & Korshin, G. V. Changes in NOM fluorescence caused by chlorination and their associations with disinfection by-products formation. Environ Sci. Technol. 43 (3), 724–729. Roccaro, P., Vagliasindi, F. G. A. & Korshin, G. V. Quantifying the formation of nitrogen-containing disinfection by-products in chlorinated water using absorbance and fluorescence indexes. Water Sci. Technol. 63 (1), 40–44. Sedlak, D. L. & von Gunten, U. The chlorine dilemma. Science 331 (6013), 42–43. Serodes, J.-B., Rodriguez, M. J., Li, H. & Bouchard, C. Occurrence of THMs and HAAs in experimental chlorinated waters of the Quebec City area (Canada). Chemosphere 51 (4), 253–263. Shah, A. D. & Mitch, W. A. Halonitroalkanes, halonitriles, haloamides, and N-nitrosamines: a critical review of nitrogenous disinfection byproduct formation pathways. Environ. Sci. Technol. 46 (1), 119–131. Siddiqui, M., Amy, G., Ryan, J. & Odem, W. Membranes for the control of natural organic matter from surface waters. Water Res. 34 (13), 3355–3370. Tung, H. H. & Xie, Y. F. Association between haloacetic acid degradation and heterotrophic bacteria in water distribution systems. Water Res. 43 (4), 971–978. Zhang, P., LaPara, T. M., Goslan, E. H., Xie, Y. F., Parsons, S. A. & Hozalski, R. M. Biodegradation of haloacetic acids by bacterial isolates and enrichment cultures from drinking water systems. Environ. Sci. Technol. 43 (9), 3169–3175. Zhao, Z.-Y., Gu, J.-D., Li, H.-B., Li, X.-Y. & Leung, K. M.-Y. Disinfection characteristics of the dissolved organic fractions at several stages of a conventional drinking water treatment plant in Southern China. J. Hazard. Mater. 172 (2–3), 1093–1099.
First received 26 February 2013; accepted in revised form 27 August 2013. Available online 30 September 2013
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A long-term prediction of domestic water demand using preprocessing in artificial neural network Sadegh Behboudian, Massoud Tabesh, Maliheh Falahnezhad and Farrokh Alavian Ghavanini
ABSTRACT Both planning and the design of water supply systems require accurate and reliable prediction of water demand. In this study, artificial neural network (ANN) was used to predict the long-term water demand to determine the relationship between dependent and independent parameters. Using the stationary chain to solve the interpolating characteristic of ANNs, the study presents a reliable approach for long-term forecasting of water demand. The purpose of this study is to provide a convenient and reliable method for long-term forecasting of urban water demand while reducing the prediction uncertainty. In order to evaluate the accuracy of the prediction, multilayer perceptron (MLP) outputs were compared with results from the linear regression model. Findings indicate that MLP is an appropriate solution for monthly long-term water demand forecasting. Furthermore, it can reduce uncertainties and significantly increase the accuracy of the long-term forecasting. Key words
| artificial neural network, long-term forecasting, preprocessing, water demand
Sadegh Behboudian (corresponding author) Farrokh Alavian Ghavanini College of Engineering, School of Civil Engineering, University of Tehran, PO Box 11155-4563, Tehran, Iran E-mail: s.behboudian@gmail.com Massoud Tabesh Center of Excellence for Engineering and Management Civil Infrastructures, College of Engineering, School of Civil Engineering, University of Tehran, PO Box 11155-4563, Tehran, Iran Maliheh Falahnezhad Department of Environmental Engineering, Graduate Faculty of Environment, University of Tehran, Ghods Street, Tehran, Iran
INTRODUCTION Prediction is a significant topic in the water industry. One
water demand and understanding its influencing factors
of the main applications of forecasting is the estimation of
are among the important steps in water crisis control and
municipal water demand. Yet, achieving the anticipated pre-
management. The effective solution not only lies in supply-
diction accuracy with regard to the forecasting trends is
ing water, but also in adopting necessary policies and
quite challenging.
schemes based on consumption patterns, and considering
Drought, population growth, and increases in per capita
factors on the demand side. For this purpose, different
consumption will give rise to a nearly global water crisis. On
econometric techniques and variables are assessed and ana-
the other hand, water is a non-renewable commodity and
lyzed. Several different data sets have been utilized, ranging
makes the problem more complicated. In this situation,
from individual household data to aggregate data, for
efforts should be made to optimize water consumption
example, cross-sectional data (Chicione & Ramammurthy
and prevent possible conflicts and quarrels to dominate
; Chen & Yang ), time-series data (Billings ;
water resources in the future. Furthermore, uneven distri-
Babel et al. ), and the most common cross-sectional
bution, either in time or resources, high evaporation rate,
time series data (Renwick & Archibald ; Mylopoulos
contamination of water resources, shortage of accurate
et al. ). The widely used variables in these studies
information, price discordance, and social problems are
include household income, size of household, density of
yet other reasons that necessitate an accurate plan in
households, gross domestic product, average or marginal
order to optimize the efficiency of water resources’ usage.
price, temperature, and precipitation (Kostas & Chrysosto-
In this way, an estimation of future water demand can
mos ; Mazzini & Montini ; Chen & Yang ).
help decision-makers to take necessary measures according
Most demand models are regression-based. They typically
to the possible crises and limitations. Forecasting domestic
use the form of Q ¼ f(P, Z), where P is the price variable
doi: 10.2166/aqua.2013.085
32
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and Z is a factor such as income, household characteristics,
predictions. To obtain the relationship between dependent
and weather (Arbues et al. ; Babel et al. ; Schleich
and independent parameters (estimating demand function)
& Hillenbrand ). In recent years, several studies have
and to forecast domestic water demand, an artificial
been made with focus on the use of artificial neural net-
neural network was used in such a way that one can forecast
works (ANNs) for short-term (hourly or daily) or medium-
long-term water demand.
term prediction (Topalli et al. ; Azadeh et al. ; Msiza et al. ; Firat et al. ). Since neural networks are trained based on a range of primary data (inputs and out-
METHODS
puts), they fail to properly predict the data outside the mentioned range (interpolation problem).
Although ANN has been mainly used for short-term forecast-
In most previous studies that have been made on neural
ing, it can be shown that it is an accurate method for long-
network forecasting purposes, a dependent variable (water
term forecasting of monthly water consumption. In this
consumption) is taken into account as an independent vari-
regard, two points should be considered: first, increasing
able (considering the time intervals). Using this procedure,
time scope in forecasting (long-term forecasting) and
the consumption value (predicted in previous stages) is
second, increasing reliability and accuracy of forecasting.
used for determining the amount of future consumption.
In this study, a regression model and the ANN model
Therefore, the error is increased at each stage and conse-
were used for modeling water demand. Predicted results
quently these models are unable to predict data more than
with both models were compared with each other. For this
a few time steps. In multivariate models, in which water con-
purpose, after estimating demand function, variables affecting
sumption is presented as a time delay, delaying parameters
per capita water demand were predicted for the desired fore-
have the greatest impact on prediction of water consumption
cast range and were given to the demand function to obtain
due to the high correlation between dependent variable and
the predicted values for per capita water demand.
intervals of the same variable which are used as an independent variable in the model. Therefore, effects of other
Regression model
variables in predicting future consumption of water cannot be assessed.
There are several variables affecting water demand, such as
Problems in long-term forecasting of water consumption
climatic, socioeconomic, and cultural variables which
using neural networks in previous studies can be summar-
should be incorporated in modeling water demand. The
ized as follows:
domestic water demand function can be estimated by differ-
• •
Interpolating nature of neural networks.
ent models (linear and nonlinear). In this approach, for
Increasing error in forecasting results due to using delay-
selecting the best model, the following criteria should be
ing values of dependent variable as independent variables.
considered:
Neglecting the effects of other variables affecting water
•
The model should be consistent with reality and in
•
The model should be used for policy-making and control-
•
consumption due to the high correlation between future water demand and consumption values in previous intervals. This study mainly intends to provide a convenient and
reliable method for predicting long-term water demand of urban areas while increasing prediction range and decreasing uncertainty of results. This paper demonstrates that the ANN approach is a good course of action for predicting
• • • • •
accordance with theoretical expectations. ling purposes. The model should be used for prediction and providence. Statistical data should be collected correctly. All assumptions are based on classic theories. The estimation method should be correct. Model coefficients should be statistically significant.
long-term monthly water demand. It also tries to solve the
The model should meet the theoretical expectations; R 2
interpolation problem of neural networks in long-term
should be high, R 2 and adjusted-R 2 should be close to each
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other. The F-statistic and the Durbin–Watson statistic verify-
and consumer services, E is the total literate individuals,
ing the entire regression must be significant.
and MT denotes the average maximum temperature.
Evaluation indices Neural network A model evaluation method is to assess its estimation perThe feed forward back propagated MLP (multilayer percep-
formance. To this effect, various criteria to assess and
tron) network was selected as the default network type for
evaluate the performance of a model in terms of data esti-
most MLPs. It has multiple neuron layers with nonlinear
mation are available. Among these, conventional criteria
transfer functions that allow the network to learn nonlinear
like correlation coefficient, the square root mean square
and linear relationships between input and output vectors.
error (RMSE), mean absolute error (MAE), and mean absol-
Learning or training in MLPs is supervised by comparing
ute percentage error (MAPE) can be mentioned:
the desired output to a particular input. Learning involves vffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi uP u n u (X Xo )2 tm¼1 p
presenting the input vectors, one at a time, at the input layer and passing them through the hidden and output layers, where the final network output is generated. At this
RMSE ¼
n
(2)
point, the network output is compared with the desired output and the difference, i.e., the error, is then calculated. If the absolute error is larger than an acceptable threshold, the error is back propagated through the network; this pro-
MAPE ¼
n 1X (Xp Xo ) n t¼1 Xo
(3)
cess adjusts weights between input and hidden layers and those between hidden and output layers using an appropriate learning method to minimize the error in repeated processing of inputs by the network. The error threshold, or acceptable limit for error, defines the accuracy of the model and depends on practical considerations. In this paper, to show the effect of variables affecting the water demand, the water demand function is estimated using
n P Xp Xo
MAE ¼ m¼1
n
(4)
in which μ is data mean, σ is the standard deviation of data, and n is the number of total data; p and o indices represent simulated and observed data, respectively.
the neural network. To obtain the relationship between dependent and independent variables and in order to predict
Preprocessing of data
the water demand, the feed forward back propagated MLP was selected as the network type (Rumelhart et al. ).
One of the most significant issues in long-term prediction
Therefore, delaying variables which decrease the accu-
with ANNs is their interpolating characteristic. To unravel
racy of forecasting were excluded from the estimation
this problem, data should be processed. After training the
model, because they increase error in long-term forecasting.
neural network with input and output data for the period
In this model, the same variables as those of the
1997–2008, it is necessary to predict input values (independent variables) for the upcoming 20 years (predicted values
regression model were used:
are presented in Table 1) and simulate the neural network Perc ¼ f(I, MP, PO, E, MT )
(1)
model with them to obtain future water demand values. Bearing in mind that the independent variables change
where Perc is per capita potable water in cubic meter, I is the
significantly over time (with respect to observed data) and
real per capita income of consumers in Rials (30,000 Rials ¼
the model is trained in the range of observed data, the
1 USD), MP is the real mean price for potable water, CPI
model would be unable to interpret these values and then pre-
(consumer price index) is the price index for commodities
dict outputs corresponding to these independent variables.
34
S. Behboudian et al.
Table 1
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method which makes variables more static and also can
Summary of statistics
Min
Max
Mean
Standard deviation
4.89
3.82
0.50
change the scale of the data. It also eliminates collinearity
Number
Demand per capita
142
Real price
142
1.62
4.80
0.69
2.74
Rials
prediction is over, it is impossible to convert output
Real income per house
142
6.044
12,808
9.247
1,827
Rials
values from the neural network to the same unit as the
Price index
142
195.80
91.23
43.20
–
2.84
Unit
m3
between variables. These removed terms must be added to
Variable
the forecasted water demand. Differencing is also another method for making time series static. However, once the
water demand, so this method was not used (in this case 35.60
the output values are from differencing ones). This preprocessing must be done before the training step in order to
To address this problem, input and output data from the training block are taken to the same scale as input
prevent saturating the neurons and also to increase the accuracy of the network.
data from the prediction period (2011–2031). In doing so, the concept of stationary chain in time series was used (Greene ). Time series are stationarized when par-
RESULTS
ameters of mean, variance, and correlation coefficients remain constant over time. The time series is made of
Study area
trend, seasonal, and irregular components. The most significant step in statistical modeling is the irregular part of
Neyshabour with a population of 205,972 is located in the
time series. Predictions based on the irregular component
center of Khorasan Razavi Province in northeastern Iran.
increase accuracy of the modeling and also produce more
The annual average temperature in Neyshabour is 14.2 C.
uniform data scale. Therefore, removing certain terms
Average annual precipitation is about 233.47 mm. A large pro-
from time series and making the data more stationary are
portion of water demand in the Neyshabour plain is supplied
essential for preparing the data series for modeling with
from wells and ground water resources. A nearly 90-cm annual
ANNs. In order to achieve a stationary condition in time
loss in the ground water level has been observed, which leads
series, first, the trends existing in data should be removed.
to increasing the water crisis in Neyshabour. The position of
Second, taking logarithm of the variables is another
Neyshabour City is shown in Figure 1.
Figure 1
|
Location of Khorasan Province and Neyshabour.
W
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Data
Model assumptions are:
The utility bill data set used for the estimation was drawn from
θ0 > 0, 0 < θ1 < 1, θ2 < 0, θ3 > 0, θ4 > 0
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the water supply company in Neyshabour during 12 years from 1997 to 2008 and contained 144 monthly observations. Infor-
Results of the demand function are shown in Table 2.
mation about residential water consumption and its respective
As the t-statistic indicates, all coefficients are significant at
price were obtained from the operators of water utilities. Real
the confidence level of 95% and estimated coefficients are per-
water price is the price determined by water utilities, while
fectly consistent with theory. The Durbin–Watson statistic
actual water price is converted from the real water price when
shows that there is no correlation between the error terms.
the price inflation is considered. The average price of water
R 2 and F-statistic values are within the desirable level and
was calculated by dividing the total revenue from the Water
the small difference between adjusted-R2 and R 2 values
and Wastewater Company in Neyshabour by the amount of
indicates the absence of additional variables in the model.
water consumption in the same month. Monthly consumer
Initial estimates of the demand function were subjected
price index, household expenditure, and the number of literate
to auto-correlation of disrupting component. AR (1) (autore-
individuals were obtained from the Central Bank of Iran and
gressive (1)) and MA (1) (moving average (1)) were used to
household expenditure is a proxy for household income. The
address this issue. The Dickey–Fuller unit-root test was per-
12-year (1997–2008) monthly temperature data were obtained
formed on all variables and, considering the fact that the
from a meteorological station inside Neyshabour. A summary
degree of all co-integrated variables is zero, there was no
of statistics for all variables is provided in Table 1.
spurious regression. In order to forecast water demand by the estimated model, independent variables should be predicted. Then,
Regression model
using these predicted values and the estimated model,
Since the Stone–Geary utility function – used for wellknown essential goods – is the most adaptable utility func-
future values for water demand can be predicted. According to Table 3, and under HADCM3 (A1B) scenario, the
tion in this regard and has a high compatibility with facts and hypotheses of this research, it was used for extracting the water demand function.
Table 2
|
Results of demand function
Based on the Stone–Geary utility function, the long-term
Coefficients
Standard error
t-statistic
p-value
water demand function was estimated for 1997 to 2008
Constant
0.866
0.7444
1.16
0.246
using time series data and economic evaluation of the ordin-
PERI
0.000222
0.00003
6.02
0.0217
ary least square method.
PINDEX
0.00898
0.0038
2.32
0.0051
E
0.00001
0.00
2.84
0.0030
MT
0.00931
0.00307
3.02
0.00
0.917
Durbin–Watson
1.7
0.913
F-statistic
248
The final model, considering maximum mean temperature and total literates, was estimated as follows: perct ¼ θ0 þ θ1
It MPt
þ θ2
POt MPt
R2
2
Adjusted R
þ θ3 Et þ θ4 MTt þ Ut
t ¼ 1, . . . , 120
(5)
It POt By substituting PERIt ¼ Pindex ¼ in MPt MPt Equation (5), for the following equation we have: perct ¼ θ0 þ θ1 Perit þ θ2 Pindext þ θ3 Et þ θ4 MTt þ Ut t ¼ 1, . . . , 120
(6)
Table 3
|
Forecast assumption variables
Number of literate
Maximum mean
Inflation
Income (economic
Water
individuals
temperature
index
growth)
price
Pars Consult Co.
A1B
15%
5%
12%
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maximum temperature values of the LARS-WG downscal-
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Results obtained from data preprocessing
ing model are predicted for the next 20 years. To this effect, the predicted values of population and total literates
The feed forward back propagated MLP is the default net-
were used. The predicted values for per capita domestic
work type for most MLPs. It has multiple layers of
income, CPI, and the average water price for 2011 to 2031
neurons with nonlinear transfer functions that allow the net-
were 12, 5 and 15%, respectively.
work to learn nonlinear and linear relationships between input and output vectors. For training the neural network,
Model accuracy
several training algorithms were used with different neurons (4–10 for each layer) and different number of layers (1–3
In order to assess the accuracy of the developed model, a
layers), and the Levenberg–Marquardt algorithm was
comparison between observed and simulated data for
selected as it produced the best result for the available
the observation period (1997–2008) was conducted.
data. The MSE performance function was selected since it
Results depict that the accuracy of the estimated model
is the default performance function for most networks.
is noticeable. Figure 2 depicts the comparison between
Three layers were implemented for the network by trial
actual water demand data and the calculated water
and error with respect to the best result (Exhaustive
demand by the estimated model. Additionally, two stat-
Search). The first layer contained nine neurons while the
istics for examining the forecasting accuracy, namely
second one had ten neurons both with TANSIG transfer
RMSE and MSE, were reported. The statistics suggest
function. The third one had one neuron (since there was
(the RMSE is 0.22 and the MSE is 0.13) that the model
only one input) with the PURELIN transfer function.
is fairly suitable for forecasting water demand in the
The network weights were initialized with values equal to inputs. Input data were separated into three blocks:
future. Obviously, for predicting per capita water demand in the
70% were used for training, 15% for validation, and 15%
future, using a neural network and a structural model, a
for testing. If the validation error was increased six times
series of dependent and independent variables were used.
sequentially, the training would be stopped. Training was
Figure 2
|
Observed and calculated data.
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restarted using network weights which had been obtained
According to the diagram, the model could forecast
from the previous run until we would reach acceptable
water demand rather well. Moreover, to assess the accuracy
results on the testing block.
of the model, MAPE, RMSE, and MSE tests and the value of correlation coefficient were used. The values of these statistics are illustrated in Table 4.
First case
These statistics indicate the good accuracy of the modelIn this case, the trend component was removed from all
ing. Therefore, the predicted values of independent variables
data in observation and prediction stages. The trend com-
were put in the simulated neural network as input data to
ponent in the observation data for water demand was:
obtain per capita water demand for the future. Once the output values were predicted using the neural
Y ¼ 0:00703t þ 3:32
(7)
network, the data should be denormalized, and the previously removed trend of water demand values should be
where t is time and Y is per capita demand. Removing the
added to the values predicted by the neural network
trend component improved the Dickey–Fuller test results.
model. Comparing ANN predicted results with predicted
According to the selection criteria, the best neural net-
values for per capita water demand obtained from the
work model in this section was found. The gradient
Stone–Geary function are shown in Figure 4. Based on pre-
descent weight/bias learning and the resilient back propa-
processing which was implemented on the input data, the
gation functions were used in the selected neural network
model could follow the general trend in water demand up
with two middle layers of nine neurons each. According to
to the 170th month. It could also simulate the seasonal
Figure 3, in order to evaluate the model, output data from
changes. As, after the 170th month, predicted input data
the test block were compared precisely with actual values.
were not in the range of data with which the network was
Figure 3
|
The comparison between observed and predicted per capita water demand for the test period (22 months).
38
Table 4
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more static and increases the modeling accuracy (Greene
The values for statistical parameters of variables
RMSE
MSE
MAPE
R
0.044
0.044
0.038
0.91
). After removal of the trend from the time series, they were normalized (standardized) for modeling. The Dickey–Fuller test results showed that taking logarithm improves test values.
trained, it fails in properly modeling the changes; therefore,
The best neural network model in this section was found
the model error increased with increasing values of indepen-
based on the selection criteria. The gradient descent with
dent variables which were increased with time as well. The
momentum weight/bias learning and one step secant back
difference between the water demand values predicted by
propagation functions were used in the selected neural net-
each model in the first 170 months was caused by errors
work with the structure of two middle layers with seven
which were generated by modeling.
neurons in the first layer and eight neurons in the second layer. Figure 5 shows the accuracy comparison of the
Second case
model in the test area with actual values.
In order that the scale of input data values in prediction
of neurons in the first and second layers. In Figure 7, the 3D
phase to be closer to data used in the training phase, logar-
surface of the correlation coefficient value and the number
ithm was taken from data, and the existing trend in
of neurons in the first and second layers clearly show that
variables was removed. Taking logarithm makes the data
the neural network in the third case (with configuration of
series smoother. Likewise, it helps a time series to be
5:7:8:1) has a greater value of R and a lower error.
Figure 6 shows the error surface in 3D and the number
Figure 4
|
The comparison between predicted per capita water demand by Stone–Geary model and ANN for the period 2011–2031.
39
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Figure 5
|
The comparison between observed and predicted per capita water demand for the test period (22 months).
Figure 6
|
The error value in 3D graph according to total of neurons on first and second layer.
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Furthermore, to assess the accuracy of the model,
These statistical values indicate that the accuracy of
MAPE, RMSE, and MSE tests were used along with the cor-
modeling is acceptable. Therefore, this simulated ANN
relation coefficient value. These statistical values are shown
can be used for predicting water demand. After obtaining
in Table 5.
the output values by the neural network, the data must be
40
S. Behboudian et al.
Figure 7
Table 5
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Long-term prediction of domestic water demand
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The correlation value in 3D graph according to total of neurons on first and second layer.
Therefore, the neural network with the 5:7:8:1 structure,
The values for statistical parameters of variables in the ANN model
logarithmic preprocessing and trend removal was recogRMSE
MSE
MAPE
R
nized as the best network. According to the predicted
0.037
0.03
0.035
0.92
values of independent variables and Figure 8, the per capita consumption for the year 2011 was estimated as 35.53 cubic meters, and for the year 2031 with a 6.48%
denormalized and the removed values of water demand
increase in per capita water demand, the per capita con-
trend should be added to the predicted values calculated
sumption was estimated as 31.79.
by the neural network. Logarithm taking should also be reversed. The comparison of ANN-predicted results with the predicted per capita water demand values derived from the
CONCLUSION
Stone–Geary function is shown in Figure 8. Based on preprocessing which was done on input data, the model
Knowing the amount of water demand is one of the impor-
could nicely predict the overall trend of the future water
tant and effective factors in water resources management.
demand according to the existing trend in descriptive vari-
To date, many reviews have been carried out in the field of
ables. Results showed that taking logarithm increases the
water demand forecast but most of these studies have focused
accuracy of prediction. According to Figure 8, in monthly
on the short-term forecast and have used self-correlation
water demand values predicted by the MLP, the effects of
models in forecasting. In this paper, to obtain the relationship
seasonal changes are visible which are created by the
between dependent and independent parameters (estimating
effect of descriptive seasonal changes, and the model also
the demand function) and long-term prediction of urban
succeeded in dealing with these changes. Results indicate
water demand, MLP was used to predict the long-term
that modeling a time series with an MLP using uncertain
water demand. For this purpose, to predict the water
components would produce better results. This is thanks
demand, effective variables for the period 1997–2008 were
to the better scaling of data to allow the ANN to address a
collected from the monthly data of Neyshabour City.
wider range. In the second case, taking logarithms improved
Maximum temperature values were predicted from
the results of the model in which the trend was removed
downscaling
from the values.
HADCM3 (A1B) scenario for the next 20 years. For this
the
model
of
LARS-WG
and
under
41
Figure 8
S. Behboudian et al.
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Comparison between predicted per capita water demand by Stone–Geary model and ANN for the period 2011–2031.
purpose, predicted population values and the number of lit-
accurate the neural network model can follow trends and
erate individuals calculated by Pars Consult Co. were used.
fluctuations.
The predicted values for per capita domestic income, CPI, and the average water price for 2011–2031 were 12, 5, and 15%, respectively. For the long-term prediction using a
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of
neural
network
were
examined
and,
by
considering the performance index, the best model was selected in each case, and output parameters were obtained through the selected model; all preprocessing was also reversed in output parameters. To scrutinize the results of modeling with the neural network, the MLP-applied forecasting results for the next 20 years were compared with the results obtained from the regression model, and it was found that the more stationary the data are, the more
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2014
Influence of porous media on intrusion rate into water distribution pipes Yan Yang, Tuqiao Zhang and David Z. Zhu
ABSTRACT Untreated water can intrude into water distribution systems through pipe leaks and cracks when negative pressure events occur inside drinking water pipelines. The orifice equation is typically used for calculation of intrusion flow rate, which ignores the impact of the soil surrounding the pipeline. This paper presents the results of an experimental study on the effect of porous media surrounding pipelines and the flow Reynolds number on intrusion flow rate for a circular orifice. The porous media, orifice size, and flow regime affect the discharge coefficient of the orifice equation. A new expression was suggested for predicting the intrusion flow rate. A discontinuity in the discharge coefficient was also found at a large Reynolds number. The effect of the pipe curvature on the discharge coefficient was found to be insignificant. Key words
| contaminant intrusion, discharge coefficient, orifice equation, porous media, water distribution system
Yan Yang College of Civil Engineering and Architecture, Zhejiang University, A810 Anzhong Building, Hangzhou 310058, China Tuqiao Zhang College of Civil Engineering and Architecture, Zhejiang University, A511 Anzhong Building, Hangzhou, 310058, China David Z. Zhu (corresponding author) College of Civil Engineering and Architecture, Zhejiang University, Hangzhou, 310058, China and Department of Civil and Environmental Engineering, University of Alberta, Edmonton, AB, Canada T6G 2W2 E-mail: david.zhu@ualberta.ca
NOMENCLATURE constants in Equation (2)
cause surrounding groundwater being intruded into the dis-
A
cross-section area of orifice
tribution systems through various types of pipe cracks and
C
fitted parameter in Equation (3)
defects (Karim et al. ). Water pipes are usually located
a
Cd discharge coefficient
below the ground with a certain thickness of soil cover
d
orifice diameter
above the pipeline. Contaminated soil and groundwater sur-
g
gravitational acceleration
rounding the pipes may contain mixtures of microbial or
ΔH difference between the external and internal pressure head
chemical contaminants (Karim et al. ; He et al. ;
i
hydraulic gradient in porous media
Besner et al. ; Payne et al. ). Even if leaking pipes
m
non-Darcy exponential
are located above the ground water table, the leak will pro-
Q
intrusion flow rate
vide a constant feed of water into the surrounding soil, while
Re Reynolds number
the contaminated water can intrude into the pipeline during
v
macroscopic velocity in porous media
negative pressure events. Intrusion of contaminants from
V
average flow velocity at the orifice
the soil-groundwater environment surrounding the pipe
ν
kinematic viscosity of water
into water distribution system has been widely recognized as a significant health threat (Karim et al. ; Besner et al. ).
INTRODUCTION
Intrusion is usually seen as a reverse leakage. Pipe leaks can occur over various kinds of defects (e.g. orifices, longi-
Low or negative pressure events may occur in drinking
tudinal cracks, circumferential cracks) (Greyvenstein &
water distribution systems (Gullick et al. ), which can
van Zyl ; Guo et al. ). In order to compute intrusion
doi: 10.2166/aqua.2013.213
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volumes, commercial surge models typically simplify the
Collins & Boxall () presents a new analytical expression
pipe defects to circular orifices, and the diameter of these
to describe the contaminants intrusion which considers the
orifices is computed based on the leakage rate of the
viscous and inertial resistance of porous media, and com-
system (Kirmeyer et al. ; Ebacher et al. ). So the
pares with the results of computational fluid dynamics
understanding of flow through circular orifices is important.
(CFD) models and experiments. The new expression indi-
The orifice equation is commonly used for the calculation of
cates a linear relationship between the flow rate and
the intrusion flow rate (Besner et al. ; Mora-Rodriguez
pressure difference when the pressure difference is small
et al. ):
or the viscous resistance of the soil significantly exceeds
pffiffiffiffiffiffiffiffiffiffiffiffi Q ¼ Cd A 2gΔH
the inertial resistance. It also reduces to the orifice equation (1)
when no resistance presents in the external porous media. It is shown that the existence of a surrounding porous media
where Q is the intrusion flow rate, Cd is the discharge coeffi-
decreases the intrusion flow rate from that predicted by
cient, A is the cross-section area of the orifice, g is the
the standard orifice equation. The analytical expression
gravitational acceleration, ΔH is the difference between the
tends to under-estimate the intrusion rate compared with
external pressure head and internal pressure head. Many
the experimental results. Mansour-Rezaei & Naser ()
factors affect the discharge coefficient, such as the ratio of
used a combination of dimensional analysis and a two-
the orifice diameter to the pipe wall thickness, the sharpness
dimensional finite element model to find the relationship
of the edge of the orifice, the roughness of the inner surface,
among the effective factors. The results show that the expo-
the type of orifice plate (plane or curved), and water
nent of pressure difference was about 2/3, and the effect of
viscosity (Brater & King ).
orifice area was lower than that in the orifice equation.
The orifice equation is commonly used to compute
The present study has three objectives. The effect of sur-
intrusion flow rate without the consideration for the sur-
face type on intrusion flow rate is studied in Experiment
rounding soil. Many researchers investigated the role of
(Exp.) 1. Pipe defects are generally located in a curved sur-
soil hydraulics on the pressure-leakage (under positive
face, while orifices are generally located in plane surface
pressure conditions in pipes) relationship. A simplistic appli-
in the traditional theory. Exp. 2 studies the effect of
cation of Darcy’s law suggests the flow rate should be
porous media surrounding pipelines, as the characteristics
linearly proportional to the pressure head in the pipe. Con-
of porous media affects the intrusion flow. The effect of
sidering the interactions of the external soil properties, the
flow at a large Reynolds number is studied in Exp. 3, as
water flow and the pipe leaks are complex, the relationship
the intrusion flow is unlikely to be laminar.
between pressure and flow rate is unlikely to be linear (Van Zyl & Clayton ). Walski et al. () compared the head loss caused by orifice losses and porous media
METHODS
losses when modeling the flow from leaks. They pointed out that orifice head loss dominates in most water distri-
Experimental apparatus
bution systems, and the orifice equation is suitable for modeling leaks for a fixed-size circular hole. Coetzer et al.
This study investigated the flow discharged through porous
() conducted an experimental study to determine the
media into an orifice on the pipe wall. The low or negative
effect of the media surrounding the pipe leakage on its
pressure inside the pipe is not directly modeled. Instead,
hydraulic behavior, and found that the flow rate for a given
the atmosphere pressure was used inside the pipe in this
pressure could be higher when the media surrounding the
study. This difference is not believed to be important as
leak is under some special conditions. This result is some-
the intrusion flow is driven by the relative pressure head
what counterintuitive, indicating the interesting interaction
difference between the inside and outside of the pipe.
of porous media and the orifice. Collins et al. () and
Figure 1(a) shows the schematics of the experimental
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relation between the pressure gradient and the flow rate, which is suitable for low Reynolds number. Under high pressure gradients, there is a nonlinear relationship between the flow rate and the pressure gradient in most surrounding soil during intrusion, thus the Darcy’s law is not valid. Different laws have been proposed like Forchheimer’s or Izbash’s law (Bordiera & Zimmer ). This study employs the Izbash equation (Izbash ) to simulate flow in porous media as it is an extension of the Darcy’s law: i ¼ avm Figure 1
|
(2)
(a) Schematics of the experimental setup (all dimensions are in millimeters); (b)
where i is the hydraulic gradient; v is the macroscopic vel-
experimental setup with porous media in Exp. 2.
ocity, a and m are constants related to the properties of setup. It consisted of a plexiglass cylindrical container filled
the porous media and the fluid, m is non-Darcy exponential.
with porous media and had an orifice at the center of the
The equation becomes Darcy’s law when m ¼ 1, and the
bottom. The container was connected to a water tank
flow is fully turbulent when m ¼ 2 (Venkataraman & Rao
which supplied the water with required pressure head. A
).
pressure sensor (Model XSE/A-H1|T2B1V0N; Westzh Tech-
Three kinds of surrounding media were used in the
nologies) with an accuracy of 0.05 kPa was used to measure
experiments: homogeneous glass beads, homogeneous
the pressure at the entrance of the orifice. A camera was
coarse sand and well-graded fine sand. The particle size of
used to record the experimental process. The outflow was
homogeneous glass beads is from 4 to 6 mm, with an average
discharged freely through the orifice. All the experiments
size of 5 mm. The particle size of homogeneous coarse sand
W
were carried out at a room temperature of 23 C.
is from 1.18 to 2.36 mm, with an average of 1.77 mm.
The height of the container was 400 mm, the inner diam-
Figure 2 shows the cumulative grain size distribution of
eter was 200 mm, and the thickness of the container bottom
the fine sand. The permeability of the three kinds of
was 5 mm. The top of the container could be opened for
porous media is tested using a similar apparatus as that of
sand loading. A curved bottom and a plane bottom were
Zhang et al. (). The non-Darcy exponential of three
used in the experiments. Half round pipe was used to form
kinds of porous media m is respectively 2 for glass beads,
a curved surface (Figure 1(a)), which had a diameter of
1.31 for the coarse sand, and 1.04 for the fine sand.
100 mm and a length of 140 mm. Two orifice sizes were used: 2.2 and 4.2 mm. The orifices were sharp-edged. The
Experimental procedures
pressure sensor was installed on the bottom of the container. The difference in the elevations of the pressure sensor and
Preparatory work included adjusting the container bottom
the orifice entrance was subtracted from the pressure
to be horizontal and packing porous media in the container.
sensor readings. Atmospheric pressure corresponds to a
The orifice was first plugged with a rubber stopper. In order
gauge pressure value of 0, thus the reading of pressure
to ensure no relative movement of particles, the maximum
sensor is equal to the difference between external pressure
hydraulic pressure in the experiments was applied to the
and internal pressure of the orifice.
porous body for more than 12 hours to make the particles compacted. Experiments were started by unplugging the
Permeability of the porous media
rubber stopper, and adjusting the water level in the water tank to the desired value. After several minutes of waiting
Flow rate through a porous media depends on permeability
to ensure that the head was steady-state, the flow rate was
and pressure gradient. The Darcy equation assumes a linear
measured by the time/weight method by collecting the
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sand or fine sand. The thickness of the glass beads layer was 85 mm and the thickness of coarse/fine sand layer was 170 mm. This arrangement could prevent small sand particles leaking into the orifice. The smooth glass beads were used as porous media in Exp. 3 for its large permeability. In China, sand is generally used as backfill material around pipes. The coarse and fine sand used in our experiments have similar properties as the sand used in China. Thus this research did not consider the effect of the soil/ clay around pipes. The physical characteristics of the porous media related to the intrusion flow is the permeability of the sand layers, not the glass beads. We have carried out experiments to test the effect of glass beads, and the results indicated that the presence of glass beads Figure 2
|
has no effect on porous media permeability.
Cumulative grain size distribution of fine sand.
outflow through the orifice over a period of time. This process and the related pressure sensor readings were
RESULTS AND DISCUSSION
recorded in the same video images. The videos recorded at 40 frames per second, so the time could be accurate to 0.025 seconds. The weight of the water was measured by
Effect of surface type
an electronic balance (with an accuracy of 0.1 g). The
Figure 3 shows the ΔH Q curves with different diameters
pressure readings were also averaged. The pressure was
and surface types for Exp. 1 without media. The curves are
increased in a stepwise fashion then decreased after reaching the maximum value in the experiments. Table 1 shows the details of the experimental conditions in this study. Exp. 1 has no porous media in the container to
fitted with Equation (1), and it can be seen that the square root relationship is suitable for both the orifice on the curved and plane surfaces. The discharge coefficient Cd are 0.69 and 0.71 – for the 2.2 mm orifice on curved and
exclude the influence of porous media. The porous media in Exp. 2 consisted of two layers as shown in Figure 1(b). The lower layer was glass beads, and the top layer was coarse Table 1
Exp. 1
|
List of experiments
Porous media
Surface type
Orifice size (mm)
No media
Curved
2.2 4.2 2.2 4.2
Plane Exp. 2
Glass beads and coarse sand
Curved
2.2 4.2 2.2 4.2
Curved
4.2
Glass beads and fine sand Exp. 3
Glass beads
Figure 3
| ΔH Q curves for different orifice diameters and surface types in Exp. 1 without media.
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plane surface. An orifice with a length (pipe thickness) to diameter ratio between 2 and 3 is called a tube, so the 2.2 mm orifice is a tube. According to Brater & King (), values of discharge coefficient for short tubes were found to vary from approximately 0.72 to 0.83. The values of Cd provided confidence that experiments results are consistent with these. Cd is 0.75 and 0.78 for the 4.2 mm orifice on curved and plane surface, respectively. They are a little larger than a typical value for an orifice, which is around 0.6. This is probably because the 4.2 mm orifice is slightly convergent, which could increase the discharge coefficient. The orifice discharge coefficient on curved surface is slightly different from that on plane surface. Brater & King () pointed out that if the plate were slightly warped inward, the coefficient of contraction would decrease. It can be seen that Cd on inward-projecting cylindrical surface is slightly smaller than that on the plane surface in our experiments, but the difference is small. Effect of porous media Figure 4(a) shows the ΔH Q curves for different orifice sizes and porous media, and Figure 4(b) shows the dependence of discharge coefficient on the Reynolds number at the orifice. The discharge coefficient Cd is calculated using Equation (1). The Reynolds number is defined by: Re ¼ Vd/ν, where V is the average flow velocity at the orifice, d is the orifice size, and ν is the kinematic viscosity of water. The range
Figure 4
|
Intrusion flow rate with different orifice diameters and porous media: (a) ΔH-Q curves; (b) Cd-Re curves.
of Reynolds number is 350 to 10,000. It can be seen from Figure 4(a) that the presence of
smaller impact on the flow rate. Cd with fine sand media
porous media changed the flow rate compared with the
is larger than that with coarse sand media. It seems coun-
no media situation, and it has a more pronounced effect
terintuitive. Particles, especially those located near the
for larger diameter orifices. In Figure 4(b), Cd is no
orifice, likely obstruct part of the orifice and modify intru-
longer a constant as in a standard orifice case. Each
sion jet behavior. The porous media has a resistance on the
curve could be divided into three regimes when Re <
flow into the orifice and also could inhibit the contraction
2000, between 2000 and 4000, and Re > 4000. These
of the flow into the orifice. This phenomenon fully illus-
values are believed to be related to the interaction of the
trates that the coupled porous media and orifice is a
porous media seepage and the orifice flow. Cd increases
complex system, and the traditional orifice equation is
with Re when Re < 2000. When Re > 4000, Cd becomes
not enough to describe the flow.
constant and is independent of Re. For the 4.2 mm orifice,
Liu et al. () demonstrated that there are similarities
the presence of porous media decreases the flow rate sig-
between flow through porous media and flow through ori-
nificantly, and Cd with coarse sand media is larger than
fices. The pressure drop for flow through the coupled
that with fine sand media, but the difference is small. For
porous media and orifice can be described by developing
the 2.2 mm orifice, the presence of porous media had
flow in short ducts and has similar predictable pressure
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Influence of porous media on intrusion rate into water distribution pipes
drop expression as that for flow through porous media. The
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Effect of the Reynolds number
orifice becomes an extension of the fluid path through the pores. It can be seen from Equation (2) that the pressure
Experiments were repeated under higher water head to
drop is proportional to the mth power of flow rate
study the effect of much larger Reynolds number. A discon-
in porous media. A relationship similar to the Izbash
tinuity can be seen from the Cd Re curve (Figure 5(a)). The
equation can be used to relate the pressure difference and
Cd suddenly changes from 0.57 to 0.46 when Re is about
flow rate:
16,000–17,000. The pattern is similar when Re is reduced from large to small. This result is in conformity with the
Q ¼ CΔH1=m
(3)
findings reported by Coetzer et al. () in their study of the effect of pressure on leakage in distribution systems.
where C is a fitted parameter, which will be discussed later.
They suggested that this discontinuity is possibly due to
When Re < 2000, the pressure drop is caused by the fric-
the separation of the fluid stream from the wall. The surrounding porous media is composed of curved
tional losses through porous media and along the wall of orifices which are mainly viscous force. This regime will
and meshed passages for flow, and the cross-sectional area
be called seepage regime here. The relationship of flow
of the passages may change. So the flow behavior is different
rate and pressure drop is mainly determined by the nature
from that without media situation. As Re increases, the
of the media, and the value of m is 1.04 for fine sand and
bending at the surface of microscopic solid causes the
1.31 for coarse sand in our experiments. When Re > 4000,
stream line to move gradually. The fluid stream may separate
flow in this regime is fully turbulent, and m ¼ 2. It is similar
from the passage wall at a certain Reynolds number. For
to the orifice equation, and could be named orifice regime.
further research on the fluid stream separation, we made
The range of Re from 2000 to 4000 is transitional regime,
an arbitrary orifice by hands on the bottom of the container
m value is uncertain in this regime. The ΔH Q curves are
to simulate the curved passage with changing cross-sectional
fitted in the seepage regime and the orifice regime, which
area, and no media is loaded in the container. The passage
is segmented according to the range of Re obtained from
had a cross-section of non-axisymmetric, and one side of
the Cd Re curves.
the inclination angle was about 10 . The surface of the pas-
W
It can be seen from Table 2 that the experimental results
sage was rough, and could be polished with sandpaper. We
fit well with Equation (3) in the seepage regime and orifice
repeated the above experiments before and after polishing.
regime. The coefficient C is related to orifice size, flow
Figure 6 shows the flow before and after the fluid stream
regime, permeability of porous media, and the local geome-
separation extracted from the experiment video with gradu-
try of the particle around the orifice. The values of C are
ally increasing Re. The jet was much more divergent
larger for a large diameter orifice. The influence of media
(Figure 6(a)) until a part of fluid stream gradually deviated
permeability to C is different in different regimes. The
from the original direction (Figure 6(b)). Finally, the jet
values of C are inversely proportional to the media per-
showed a constrictive appearance, and a vena contracta
meability
are
appeared downstream of the orifice (Figure 6(c)). This
approximately equal for different media in the orifice
shape was maintained with further increase of the Reynolds
regime.
number. Figure 5(b) shows the Cd Re curve of the
Table 2
|
in
the
seepage
regime,
and
they
The fitting equations of ΔH-Q curves with different porous media
Media
Orifice size (mm)
Seepage regime
R2
Orifice regime
R2
Course sand
2.2 4.2
Q ¼ 19:67ΔH1=1:31 Q ¼ 68:34ΔH1=1:31
0.995 0.996
Q ¼ 10:78ΔH1=2 Q ¼ 29:39ΔH1=2
0.999 0.997
Fine sand
2.2 4.2
Q ¼ 47:39ΔH1=1:04 Q ¼ 125:39ΔH1=1:04
0.966 0.984
Q ¼ 12:15ΔH1=2 Q ¼ 29:13ΔH1=2
0.999 0.998
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experiment results before and after polishing. After the fluid stream separation, the discharge coefficient decreased as the flow contracted. As Re decreased with the decrease in the flow rate, Cd still remained the value after the separation. Thus there was a range of Re corresponding to two values of Cd. The surface of the passage became smoother after being polished, the friction head loss reduced. As a result, Cd increased slightly compared to the value before polishing. The Reynolds number corresponding to the discontinuity was smaller after being polished, which indicates that the fluid stream separation is related to the roughness of the passage.
CONCLUSIONS This study investigated the influence of porous media on the intrusion flow rate through orifices. The intrusion is assumed to occur under steady-state conditions, flow through orifices discharging free liquid jets into air. The porous media in the surrounding environment of the orifice is fully-saturated, homogeneous and isotropic. Experimental results show that the traditional orifice equation is suitable for both the orifice on curved surface and plane surface when there is no porous media surrounding the orifice. Figure 5
|
Cd-Re curves: (a) with glass beads as porous media for a 4.2 mm orifice; (b) before and after polishing for an arbitrary orifice with no porous media.
The orifice discharge coefficient on the inward curved surface is smaller than that on the plane surface, but the difference is relatively small. The presence of porous media could change the discharge coefficient and added dependencies on the orifice size, flow regime, and permeability of porous media. A function similar to the Izbash equation is suggested for describing the relationship of the pressure head difference and the flow rate, which fits well with the experimental data both in seepage regime and orifice regime. This expression describes well the complex nature of the flow where the flow is impacted by both the porous media and the orifice. It should be pointed out, however, that further research is needed to develop a general equation for practical use. There is a discontinuity in the discharge coefficient at large Reynolds number (Re > 10,000) when the porous
Figure 6
|
Flow forms before and after fluid stream separation for an arbitrary orifice with no porous media (the arrows indicate the location of the orifice).
media is composed of curved and meshed passages for flow. The value of discharge coefficient may change due to
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Influence of porous media on intrusion rate into water distribution pipes
the movement of the stream line, leading to changes in the flow rate. This is different from the continuum hypothesis. Previous research simplified the porous media as a continuous media is inappropriate.
ACKNOWLEDGEMENTS Financial support was received from the Nation High-Tech R&D Program (863) of China (2012AA062608), the Important National Science and Technology Specific Projects (2011ZX07301-004), and the Program for Zhejiang Leading Team of S&T Innovation (2010R50037).
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Greyvenstein, B. & Van Zyl, J. E. An experimental investigation into the pressure–leakage relationship of some failed water pipes. J. Water Supply Res. T. 56 (2), 117–124. Gullick, R. M., LeChevallier, M. W., Case, J., Wood, D. J., Funk, J. E. & Friedman, M. J. Application of pressure monitoring and modelling to detect and minimize low pressure events in distribution systems. J. Water Supply Res. T. 54 (2), 65–81. Guo, S., Zhang, T., Zhang, Y. & Zhu, D. Z. An approximate solution for two-dimensional groundwater infiltration in sewer systems. Water Sci. Technol. 67 (2), 347–352. He, X. Q., Cheng, L., Zhang, D. Y., Li, W., Xie, X. M., Ma, M. & Wang, Z. J. First molecular detection of group A rotaviruses in drinking water sources in Beijing, China. Bull. Environ. Contam. Toxicol. 83, 120–124. Izbash, S. O Filtracii V Kropnozernstom Materiale. Leningrad, USSR. Karim, M. R., Abbaszadegan, M. & Lechevallier, M. Potential for pathogen intrusion during pressure transients. J. Am. Water Works Assoc. 95 (5), 134–146. Kirmeyer, G. J., Friedman, M., Martel, K., Howie, D., LeChevallier, M., Abbaszadegan, M., Karim, M., Funk, J. & Harbour, J. Pathogen Intrusion into the Distribution System. American Water Works Association Research Foundation, Denver, CO. Liu, S., Afacan, A. & Masliyah, J. H. A new pressure drop model for flow-through orifice plates. Can. J. Chem. Eng. 79, 100–106. Mansour-Rezaei, S. & Naser, G. H. Contaminant intrusion in water distribution systems: an ingress model. In: World Environmental and Water Resources Congress 2012. Albuquerque, New Mexico, USA, pp. 3002–3010. Mora-Rodriguez, J., Lopez-Jimenez, P. A. & Ramos, H. M. Intrusion and leakage in drinking systems induced by pressure variation. J. Water Supply Res. T. 61 (7), 387–402. Payne, S. J., Besner, M. C., Lavoie, J., Krentz, C., Hansen, L. T., Friedman, M., LeChevallier, M. W., Prevost, M. & Gagnon, G. A. Molecular techniques and data integration: investigating distribution system coliform events. J. Water Supply Res. T. 59 (5), 298–311. Van Zyl, J. E. & Clayton, C. R. I. The effect of pressure on leakage in water distribution systems. P. I. Civil Eng.-Water M. 160 (2), 109–114. Venkataraman, P. & Rao, P. R. M. Darcian, transitional, and turbulent flow through porous media. J. Hydraul. Eng. 124 (8), 840–846. Walski, T., Bezts, W., Posluszny, E. T., Weir, M. & Whitman, B. E. Modeling leakage reduction through pressure control. J. Am. Water Works Ass. 94 (4), 147–155. Zhang, Y., Liu, W., Shao, W. & Yang, Y. Experimental study on water permittivity of woven polypropylene geotextile under tension. Geotext. Geomembranes 37, 10–15.
First received 12 June 2013; accepted in revised form 3 September 2013. Available online 8 October 2013
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Optimal sensor placement for event detection and source identification in water distribution networks Shuming Liu and Pierre Auckenthaler
ABSTRACT This study focuses on the optimization of sensor placement with respect to the source identification and event detection. A multi-objective algorithm is used to solve the optimization problem. The numbers of possible source nodes for contamination events associated with the solutions on the Pareto fronts from the proposed method and benchmark method are calculated under the same configuration and compared. The comparison showed that the proposed method performs better than the benchmark method in detecting a contamination event and identifying its possible source. Key words
| multi-objective genetic algorithm, nodal demand uncertainties, sensor placement, source identification
Shuming Liu (corresponding author) Pierre Auckenthaler School of Environment, Tsinghua University, Beijing 100084, China E-mail: shumingliu@tsinghua.edu.cn Shuming Liu Tsinghua University-VEOLIA Environment Joint Research Center for Advanced Environmental Technology, Tsinghua University, Beijing 100084, China
INTRODUCTION Accidental contamination or malicious attack on a water
). It also attracted much interest and several methods
distribution network can have severe effects on the health
have been developed to solve it, especially in recent
of the population relying on this water source. These
BWSNs. For example, Cristo & Leopardi () formulated
events can potentially be detected by a network of online
it as an optimization problem, linearized using the water
sensors. In order to reduce the exposure to contaminated
fraction matrix concept. Liu et al. () solved this problem
water, it is important to design a methodology to efficiently
using an adaptive dynamic optimization technique. Wang &
place the sensors (Ostfeld et al. ). Once a contamination
Harrison (, ) applied Bayesian analysis to solve the
event is detected, the next important step is to identify the
source identification problem, especially in the condition
source of this event.
of stochastic variation of water demand. Shen & McBean
The sensor placement problem is concerned with locating an array of sensors in a network capable of detecting the
() investigated the false negative/positive issues in contaminant source identification.
presence of a contaminant if an event occurs. Since the first
Generally, these two problems were solved separately.
article by Lee & Deininger (), the sensor placement pro-
Only a few researchers have attempted to investigate them
blem sparked significant research, most notably, leading to
jointly. In 2006, Preis & Ostfeld observed this dependency
the Battle of the Water Sensor Networks (BWSNs) (Ostfeld
and proposed a method to optimize the sensor layout with
et al. ). Due to its complexity, it is often treated as a
respect to source identification (Preis & Ostfeld ).
multi-objective optimization problem. Optimization criteria
More recently, Tryby et al. () represented the water dis-
may include population exposed, time to detection,
tribution system as a linear system and optimized the
volume of contaminated water consumed, number of
positions of the sensors in order to improve the conditioning
failed detections, and length of pipe contaminated (Berry
of the matrix. This paper presents a new method to focus on
et al. ). These objectives are mostly related to the sen-
the optimization of sensor placement with respect to source
sor’s ability in event detection.
identification and event detection. The proposed method uti-
The source identification problem is concerned with identifying the contaminant source location (Tryby et al. doi: 10.2166/aqua.2013.106
lizes different objectives compared with conventional methods.
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alarm threshold. The values of Δ adopted are 10% and
METHODOLOGY
þ10%. Ideally, all concentration values from all nodes at every
Nodal demand uncertainty
time step, for all simulations, should be recorded. HowIn the operation of a network, uncertainties might come
ever, such records would lead to a large amount of data,
from nodal demand, sudden loss of electricity, etc. For sim-
much too large to be used efficiently, even for small net-
plification, only the nodal demand uncertainty is considered
works (Krause et al. ). Instead, it can record the
in this research, which is realized by multiplying the base
time of first detection of the simulated event by each
demand with a random demand multiplier. A truncated
node to reduce computing load (Krause et al. ),
Gaussian probability function (PDF) is employed to gener-
which is the principle used in this research. The time at
ate the random demand multiplier (Babayan et al. ).
which a sensor s (at node s) detects the event e under
This is expressed as:
the nodal demand configuration i is called the detection time t(e, s, i). t(e, s, i). is calculated to be the shortest
2 1 2 pdf ¼ pffiffiffiffiffiffi exp ((x E) =2σ ) x 1 σ 2π
(1)
travel time of water parcels from the contamination event node to the sensor node, which is used as an indicator to identify the contamination source of event e for sensor at
where E and σ are given mean and standard deviation. In
node s. In addition, the interval of detection time is
this research, the values of σ are 0, 0.1 and 0.2, and E ¼ 0.
denoted [Tmin (e, s); Tmax (e, s)], in which Tmin (e, s) ¼
The random nodal demand is calculated as:
min t(e, s, i) Tmax (e, s) ¼ max t(e, s, i). In the case where the contaminant concentration is lower than the sensor’s
w(k, j) ! wb (k, j) M(k, j)
(2)
alarm threshold, it is considered ‘non-detection’. If the event goes undetected during the whole simulation, it is
where w(k, j) is the demand at network junction k at time
defined as t(e, s, i) ¼ 1.
step j, wb(k, j) is the base demand at network junction k at time step j, M(k, j) is the demand multiplier at network junc-
Optimization
tion k at time step j. The sensor placement problem is configured to be a multiSimulation of contamination data
objective optimization problem. The objectives are to (1) maximize the probability of detection and (2) minimize
Features of contamination events, including contaminant
the overlay of interval of detection time. To solve the optim-
type, duration, contaminant magnitude and starting time,
ization problem, a NSGA-II method is employed. NSGA-II
may have impacts on source identification. For simplifica-
is an algorithm proposed by Deb et al. (), which has
tion, it is assumed that the contamination is a single
been broadly used in water distribution area (Preis & Ost-
conservative injection event with specified unit duration
feld ; Liu et al. ).
and could happen at any point of the discretized timeline in the first 12 hours. Such an event is noted e and the
First objective: maximize the probability of detection
set of all possible events is noted E. The type of sensors considered is with an alarm threshold d. If the indicator
The first objective is to maximize the probability of detec-
concentration (for example, dissolvedoxygen) is below d,
tion, which is defined as the ratio of detected events
no alarm will be triggered. If the concentration goes
relative to all simulated events:
above d, the sensor immediately reports an abnormal situation.
The
impact
of
alarm
threshold
on
model
performance is examined by adding a shift Δ to the original
fitness1 ¼
number of detected events total number of events
(3)
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A greater value of fitness1 suggests an event e can be
Second objective: minimize the overlay of interval of detection time
detected with high probability, while a greater value of fitness means a higher overlay of detection time and lower accuracy of
A single event will give a deterministic value of the detection
source identification. In the case of non-detection, a large
time for a sensor. In this case, it is possible to distinguish two
number, for example 1010 in this research, is set to fitness2 as
events by comparing the detection times. In the case where
a penalty.
the detection times are identical, the two events can be distinguished by further comparing the sensor measurements. In the situation of detection, times and sensor measurements are both identical, the two events are the same from the sensor’s point of view and will not be distinguished. This simple dichotomy disappears when nodal demand uncertainties are considered, because the detection time of an event by a sensor becomes a set of possible times. The set of possible detection times of two events can be identical, completely different or partially overlapped. The partial overlap means that under some nodal demand configurations, the two events can be distinguished by the sensors. While under other nodal demand configurations, they cannot be distinguished. Therefore, the second objective is to minimize the overlap of internal of detection time. A value v(s, e1, e2) is
Comparison benchmark For comparison, another set of solutions is yielded through optimization with respect to probability of detection (the first objective defined above) and time to detection (objective used in conventional methods). Time to detection is defined as the value of the difference between the contamination time (Tevent) and the median value of the detection interval for the first sensor to detect the event. Small fitness values suggest small detection times: fitness3 (S) ¼ min
X
(Tmin þ 0:5 (Tmax Tmin ) Tevent )
(7)
first calculated, corresponding to the ability for a single Therefore, the benchmark optimal sensor placement
sensor s to distinguish between two events e1 and e2: v(s, e1 , e2 ) ¼
1 overlap overlap þ 2 l1 l2
l1 ¼ Tmax (e1 , s) Tmin (e1 , s) l2 ¼ Tmax (e2 , s) Tmin (e2 , s)
problem has two objectives: maximization of detection probability and minimization of detection time. (4)
These two multi-optimization problems share one same objective. However, the second objective is different. To facilitate the comparison, after the optimization problem is solved, the numbers of possible source nodes for con-
where l1 and l2 are the length of the interval of detection time for the first and second event, l1 ≠ 0, l2 ≠ 0, Tmax > 0, Tmin > 0,
tamination events associated with the solutions on the Pareto fronts from both methods are calculated under the
overlap is the length of the overlap between the interval of
same configuration as the one used in the optimization
detection time.
processes.
The value attributed to a single sensor can be extended to a set of sensors by taking the minimum value from each sensor: Source identification v(S, e1 , e2 ) ¼ min v(s, e1 , e2 ) s∈S
(5) At time t, if sensor s1 is triggered off and sensor s2 is not,
By summary, the optimization problem for optimal sensor placement is formulated as follows:
and 0 < Tmin(ex, s2) Tmax(ex, s2) Tmin(ex, s1), node x is excluded from the potential contamination source. Otherwise, x is a possible contamination source. At time t þ t0 ,
number of detected events total number of events XX Minimize fitness2 (S) ¼ v(S, e1 , e2 )
if sensor s2 is triggered off and 0 < Tmin(ex, s2) Tmax(ex,
Maximize fitness1 ¼
(e1 ≠ e2 ;
e1 , e2 ∈ E)
s2) t0 , node x is excluded from the potential contamination source. Otherwise, x is a possible contamination (6)
source.
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CASE STUDY
RESULTS
The methodology discussed above was implemented using
Figure 1 presents the Pareto fronts obtained using the pro-
Matlab. The hydraulic and water quality simulations were
posed method. It reveals that nodal demand uncertainty
performed using the EPANET Program’s toolkit (Rossman
does not affect detection probability significantly. However,
). Example network Net 3 from EPANET was utilized
for a given number of sensors, with increasing of uncer-
to demonstrate the proposed method. For simplification, a
tainty, for the same detection probability, the identification
base demand pattern is applied to all nodes.
fitness increases, which suggests a decrease of accuracy of
Simulations were carried out with different levels of
source identification. Meanwhile, as shown in Figure 2,
uncertainties of the nodal demand (σ: 0, 0.1 and 0.2) and
when the alarm threshold decreases, the detection prob-
alarm threshold (Δ: 10%, 0%, þ10%). For each level of
ability and the overlay of interval of detection time
uncertainties, the optimization process was conducted for
increase, which means a contamination event can be
three, six and 12 sensors, respectively. The injection dur-
easier to be detected, but with lower identification accuracy.
ation is set to 1 minute. The nodal demand w is
In contrast, for a greater alarm threshold value, a contami-
calculated using Equation (2). Based on the initial calcu-
nation event can be more difficult to be detected, but with
lation of the flow velocity, water quality simulation length
higher identification accuracy. These two findings suggest
was set to 24 hours to ensure all contaminant is spread
the proposed method is sensitive to nodal demand and
over the whole network.
alarm threshold.
Figure 1
|
Pareto front from the proposed method (nodal demand).
Figure 2
|
Pareto front from the proposed method (alarm threshold).
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The possible source nodes for contamination events
Figure 4 presents the Pareto front obtained with six
associated with the solutions on the Pareto fronts from the
sensors, as well as the explicit placement of the sensors
proposed and benchmark methods are calculated and pre-
for four different sensors sets. The solutions present a gra-
sented in Figure 3. Generally, for the same number of
dual evolution going from the most compact sensor
possible contamination sources, the results of the proposed
placement (Figure 4(a)), giving a better identification accu-
method show higher detection probability than the one from
racy with low detection probability, to the most scattered
the benchmark method. Meanwhile, for a given contami-
one, giving a worse identification accuracy with high
nation event, the proposed method reports a lower
detection probability (Figure 4(d)). A compact sensor pla-
number of possible contamination sources than the bench-
cement can identify more accurately the source of a
mark method with the same detection probability. This
contamination event but will miss many events. On the
suggests that the proposed method performs better than
contrary, a well spread out sensor network can detect an
the benchmark method in event detection and source
event with higher probability, while accuracy of source
identification.
identification is low.
Figure 3
|
Possible contamination sources from proposed method and benchmark method.
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well spread out sensor network can detect an event with higher probability, while accuracy of source identification is low. 4. Many factors may have impacts on the model’s performance. This research only simply examined nodal demand and alarm threshold. The impact of the profile of contamination event on method performance, including injection duration and contaminant magnitude, etc., and the use of detection time and sensor measurement to differentiate events should be investigated in future research.
ACKNOWLEDGEMENTS The authors express their thanks to the China Major Water Project (2012ZX07408-002) and Tsinghua Independent Research Grant for their financial support. The authors would like to thank the two anonymous reviewers for their valuable comments on this manuscript.
REFERENCES
Figure 4
|
Four sample solutions of the Pareto front obtained for six sensors with σ ¼ 0.1.
CONCLUSIONS 1. The proposed method employs detection probability and overlap of detection time as objectives, which differentiates it from the conventional methods. By taking the overlap of detection time into consideration, the proposed method performs well, both in detecting a contamination event and identifying its possible sources. 2. The proposed method is sensitive to nodal demand and sensor’s alarm threshold. Increase of nodal demand uncertainty and decrease of alarm threshold both could blur the accuracy of source identification. 3. A compact sensor placement will make use of the redundancy between the sensors to identify more accurately the source of a contamination event. On the contrary, a
Babayan, A., Kapelan, Z., Savic, D. & Walters, G. Least-cost design of water distribution networks under demand uncertainty. J. Water Resour. Plann. Manage. 131 (5), 375–382. Berry, J. W., Fleischer, L., Hart, W. E., Phillips, C. A. & Watson, J. P. Sensor placement in municipal water networks. J. Water Resour. Plann. Manage. 131 (3), 237–243. Cristo, C. D. & Leopardi, A. Pollution source identification of accidental contamination in water distribution networks. J. Water Resour. Plann. Manage. 134 (2), 197–202. Deb, K., Pratao, A., Agarwal, S. & Meyarivan, T. A fast and elitist multiobjective genetic algorithm: NSGA-II. IEEE Trans. Evol. Comput. 6 (2), 182–197. Krause, A., Leskovec, J., Guestrin, C., VanBriesen, J. & Faloutsos, C. Efficient sensor placement optimization for securing large water distribution networks. J. Water Resour. Plann. Manage. 134 (6), 516–526. Lee, B. H. & Deininger, R. A. Optimal locations of monitoring stations in water distribution system. J. Environ. Eng. 118 (1), 4–16. Liu, L., Ranjithan, R. S. & Mahinthakumar, G. Contamination source identification in water distribution systems using an adaptive dynamic optimization procedure. J. Water Resour. Plann. Manage. 137 (2), 183–192.
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Liu, S., Liu, W., Chen, J. & Wang, Q. Optimal locations of monitoring stations in water distribution systems under multiple demand patterns: a flaw of demand coverage method and modification. Front. Environ. Sci. Eng. 6 (2), 204–212. Ostfeld, A., Uber, J. G., Salomons, E., Berry, J. W., Hart, W. E., Phillips, C. A., Watson, P.-J., Dorini, G., Jonkergouw, P., Kapelan, Z., Pierro, F., Khu, S.-T., Savic, D., Eliades, D., Polycarpou, M., Ghimire, S. R., Barkdoll, B. D., Gueli, R., Huang, J. J., McBean, E. A., James, W., Krause, A., Leskkovec, J., Isovitsch, S., Xu, J., Guestrin, C., VanBriesen, J., Small, M., Fischbeck, P., Preis, A., Propato, M., Piller, O., Trachtman, G. B., Wu, Z. Y. & Walski, T. The battle of the water sensor networks (BWSN): a design challenge for engineers and algorithms. J. Water Resour. Plann. Manage. 134 (6), 556–568. Preis, A. & Ostfeld, A. Optimal sensors layout for contamination source identification in water distribution systems. In: Proc. 8th Annual Water Distribution Systems Analysis Symp. ASCE, Reston, VA.
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Preis, A. & Ostfeld, A. A genetic algorithm for contaminant source characterization using imperfect sensors. Civil Eng. Environ. Syst. 25 (1), 29–39. Rossman, L. A. The EPANET programmer’s toolkit for analysis of water distribution systems. In: Proc. Annual Water Resources Planning and Management Conf. ASCE, Reston, VA. Shen, H. & McBean, E. False negative/positive issues in contaminant source identification for water-distribution systems. J. Water Resour. Plann. Manage. 138 (3), 230–236. Tryby, M. E., Propato, M. & Ranjithan, S. R. Monitoring design for source identification in water distribution systems. J. Water Resour. Plann. Manage. 136 (6), 637–646. Wang, H. & Harrison, K. Bayesian update method for contaminant source characterization in water distribution systems. J. Water Resour. Plann. Manage. 139 (1), 13–22. Wang, H. & Harrison, K. Improving efficiency of the Bayesian approach for water distribution contaminant source characterization with support vector regression. J. Water Resour. Plann. Manage. 140 (1), 3–11. doi:10.1061/(ASCE) WR.1943-5452.0000323.
First received 5 June 2013; accepted in revised form 19 September 2013. Available online 31 October 2013
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Effects of the interaction between Microcystis aeruginosa and nitrobenzene on coagulation-sedimentation performance Zhiquan Liu, Zhenling Hou, Hua Ma, Zhenqiang Fan, Zhiwei Zhao, Dongmei Liu and Fuyi Cui
ABSTRACT It is rarely reported that the interaction between xenobiotics and algae may cause potential water quality risks and affect the drinking water treatment process. In the present study, a bench-scale jar test was performed to investigate the effects of the interaction between nitrobenzene (NB) and Microcystis aeruginosa on the performance of coagulation-sedimentation by comparing differences in turbidity, optical density at 680 nm (OD680), trihalomethane formation potential (THMFP) and microcystin-LR (MC-LR) in an M. aeruginosa solution with or without NB. The results indicated that the quality of M. aeruginosa-containing water can be improved significantly by coagulationsedimentation, and all of the removal rates were more than 80%. The presence of NB did not affect the performance of coagulation-sedimentation directly. However, the interaction between NB and M. aeruginosa did change the characteristics of the raw water and affect the performance of coagulation-sedimentation. At a non-lethal concentration, NB did not inhibit the growth of M. aeruginosa but weakened the zeta potential of M. aeruginosa, which enhanced the removal of turbidity. The products of NB degradation by M. aeruginosa cause an increased THMFP in extracellular organic matters, which cannot be removed by coagulation-sedimentation efficiently, increasing the risk of disinfection by-products formation in the following disinfection unit. Key words
Zhiquan Liu Zhenling Hou Hua Ma Zhenqiang Fan Zhiwei Zhao Dongmei Liu Fuyi Cui (corresponding author) State Key Laboratory of Urban Water Resource and Environment, Harbin Institute of Technology (SKLUWRE, HIT), PO Box 2650, Harbin 150090, China E-mail: hit_cuifuyi@hotmail.com Zhiquan Liu Department of Environmental Engineering and Global Water Quality Research Center, National Cheng Kung University, Tainan 70101, Taiwan Zhenling Hou Changchun Institute of Urban Planning & Designing, Changchun 130021, China
| algae, coagulation, sedimentation, THMFP, xenobiotics
INTRODUCTION Eutrophication and xenobiotic pollution are two of the
water treatment process and worsen the effluent water
most common problems in the aquatic environment.
quality. The characteristics and effects of individual algal
Sometimes,
or organic problems on water treatment plants have
these
two
problems
may occur
simul-
taneously. An official Chinese investigation (Ministry of
been well studied (Takaara et al. ; Tian et al. ;
Environmental Protection of the People’s Republic of
Shen et al. ; Zamyadi et al. ). However, the effects
China ) indicates that of the 26 total monitored
of the interaction between xenobiotics and algae are
large lakes and reservoirs, 14 (53.8%) face a eutrophica-
rarely reported.
tion problem and 16 (61.5%) face a xenobiotic pollution
Xenobiotics can inhibit the growth and metabolism of
problem. The study also indicates that Taihu Lake,
algae (Tukaj ; Andreozzi et al. ), while algae and
Chaohu Lake and Dianchi Lake are contaminated by a
cyanobacteria have the ability to adsorb or degrade xeno-
combination of xenobiotics and algae (including cyano-
biotics (Semple et al. ). Both interactions depend on
bacteria) in the summer. When these lakes are used as
the physical and chemical properties of the xenobiotics
drinking water sources, the pollutants can affect the
and the species of algae.
doi: 10.2166/aqua.2013.081
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Due to the interaction between xenobiotics and algae, the
lowest temperature) for M. aeruginosa blooms. Alkalinity
characteristics of the raw water may change, hence affecting
and pH can affect the hydrolysis of coagulants and the per-
the performance of water treatment plants. Our previous
formance of coagulation-sedimentation (Gottfried et al.
study (Liu et al. ) indicated that the presence of nitrobenzene
). Because the low alkalinity in M. aeruginosa solutions
(NB) can enhance the protein productivity of Microcystis aeru-
limited the coagulation efficiency (less than 70% for the
ginosa and result in an increased yield of trihalomethane
removal of OD680), 106 mg/L sodium carbonate (equivalent
formation potential (THMFP) by M. aeruginosa. However, it
to 100 mg/L alkalinity as CaCO3) was added to all the
is still not clear whether increased THMFP productivity will
samples before the coagulation-sedimentation experiment.
cause an increased risk of disinfection by-products formation
Aluminum sulfate, ferric chloride and polyaluminum chlor-
in the effluent of water treatment plants or not.
ide (PAC) were used as the coagulants. Following the
In the present study, NB, a typical industrial material
addition of coagulant, the waters were subjected to rapid
widely observed in the aquatic environment (Gao et al.
mixing for 1 min at 250 rpm, flocculation for 14 min (4 min
), and M. aeruginosa, a common dominant species of
at 100 rpm and 10 min at 40 rpm), and settling for 30 min.
cyanobacteria in eutrophic lakes and reservoirs that can
A pre-experiment (Figure S1, supplementary data, avail-
release microcystins (MCs), were selected as the representa-
able online at http://www.iwaponline.com/jws/063/081.
tive pollutants. A bench-scale jar test was conducted to
pdf) showed that at the coagulant dosage optimized for tur-
evaluate the effects of the interaction between NB and M. aer-
bidity, other water quality parameters of the settled water
uginosa on the performance of coagulation-sedimentation.
also approximated optimal values. Thus, in this study, all of the presented data were obtained at the coagulant dosage optimized for turbidity (the residual turbidity with
MATERIALS AND METHODS
different coagulant dosages can be found in Figure S2, available online at http://www.iwaponline.com/jws/063/081.
M. aeruginosa culturing
pdf). All of the jar tests were conducted in triplicate, and the arithmetic mean (±SD) was used as the final value.
Axenic M. aeruginosa (FACHB-930) was purchased from the Institute of Hydrobiology at the Chinese Academy of
Analytical methods
Sciences but was still treated by Semple & Cain’s () method to exclude microbial contamination. The stock cul-
The algal density was monitored by spectrophotometry at a
ture and the experimental culture were incubated under the
wavelength of 680 nm (OD680, UV759S, INESA instrument
W
designed conditions (BG11 medium, 25 C) as described in
Co. Ltd, China), and cell number counting was performed
our previous publication (Liu et al. ), and the com-
with a microscope (Olympus BX41, Olympus Optical Co.,
ponents of BG11 medium have been listed in supporting
Ltd, Japan) according to the method adopted by Ma et al.
information (Tables S1 and S2, available online at http://
(). There was a significant linear regression between
www.iwaponline.com/jws/063/081.pdf).
OD680 and cell density (Figure S3, available online at http://www.iwaponline.com/jws/063/081.pdf).
Jar test
We
used
OD680 to study the removal rate of cell density, and checked the initial cell density by microscope analysis before the
The bench-scale coagulation-sedimentation experiments
coagulation-sedimentation experiment to ensure consistent
were conducted using a standard jar-test unit (ZR2-6, Fuhua
initial conditions in different batch experiments.
Co. Ltd, China) consisting of six 2-L glass jars. The glass
THMFP was measured by gas chromatography with an
jars were used to minimize the adsorption of organic com-
electron capture detector (Agilent 7890N) according to
pounds by the containers. Due to the low room temperature
Liu’s method (). An excess chlorine dosage (1,600 mg/L)
W
(14–18 C), a water bath was used to maintain the water temp-
was applied to ensure that all the THMFP could be oxidized
erature at 25 ± 1 C, which is a necessary condition (the
to form THMs, independent of the actual chlorine dosage
W
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used during disinfection; the results do not reflect the real pro-
NM5 samples (i.e. NB concentration of 83.5 μg/L and cell
duction of THMs under actual conditions.
density of 2.1 × 108 cells/L), was also subjected to the jar
The intracellular microcystin-LR (MC-LR) and extracellular MC-LR were extracted and measured according to
test. For NMf, it was assumed that there was no interaction between NB and M. aeruginosa in the mixture.
Meriluoto & Spoof’s (a, b) method, but the extracellular MC-LR was undetectable (below 1 μg/L) in most instances because of the low death rate of M. aeruginosa in the exponential growth phase and the low release rate of
RESULTS AND DISCUSSION
MC-LR by the dead cells. Briefly, for the intracellular MC-LR, the algal cells were harvested by filtration (0.45-μm glass fiber filters, Taoyuan Co. Ltd, China),
Effect of NB on the performance of coagulationsedimentation
broken by freeze-thawing, and extracted by 75% methanol, while the extracellular MC-LR in the filtrate was extracted by solid phase extraction. Both the intracellular MC-LR and extracellular MC-LR were analyzed by high performance liquid chromatography. Turbidity was measured using a HACH 2100P turbidimeter. The NB concentration was measured by high performance liquid chromatography (Waters e2695) according to Liu’s () method. The UV absorbance at 254 nm (UV254) was measured using a spectrophotometer (UV759S, INESA Instrument Co. Ltd, China) after the samples were filtered through 0.45-μm filters. Dissolved organic carbon (DOC) was measured using a Shimadzu TOC 5000 analyzer (Shimadzu, Kyoto, Japan) after filtration by 0.45-μm filters. Zeta potential (ZP) was measured using a Zetasizer Nano-Z (Malvern Instruments, Worcestershire, UK). Total alkalinity was measured by the Gran titration method.
The removal rates of turbidity, OD680, total THMFP, THMFP in the extracellular organic matter (EOM) and intracellular MC-LR in the M. aeruginosa solution and in NMf were investigated, and the results are presented in Figure 1. The quality of the water containing M. aeruginosa was significantly improved by coagulation-sedimentation at an optimized dosage of coagulant. The removal rates of all five parameters (Figure 1) were higher than 80%. In this experiment, there were no other impurities in the M. aeruginosa solution except the cyanobacteria cells and their secretions, which caused the turbidity in the water (Divakaran & Pillai ). With the good sedimentation of M. aeruginosa cells, intracellular MC-LR and turbidity were also removed. Extracellular MC-LR in the settled water was undetectable, which indicated that coagulationsedimentation would not destroy the M. aeruginosa cells
EXPERIMENT A mixture of NB and M. aeruginosa (NM5), which was incubated for 5 days with an initial NB concentration of 160 μg/L and an initial cell density of 1.0 × 108 cells/L, was subjected to the jar test. The final density of M. aeruginosa in NM5 was 2.1 ± 0.1 × 108 cells/L, and the finial NB concentration was 83.5 ± 2.2 μg/L. An M. aeruginosa solution with the same initial cell density (1.0 × 108 cells/L) and an NB solution (without M. aeruginosa) with the same initial NB concentration (160 μg/L) were incubated for 5 days and then used as control samples. A fresh mixture of NB and M. aeruginosa without incubation (NMf ), which contained the same NB concentration and cell density as the
Figure 1
|
Results of coagulation-sedimentation of M. aeruginosa solution and the fresh mixture of NB and M. aeruginosa without incubation (NMf ). Coagulant: Al2(SO4)3 at the optimized dosage of 20 mg Al2O3/L; 25 ± 1 C. W
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and result in a release of intracellular MC-LR into solution
of colloidal materials and the charge complexation/
as reported by Chow et al. (). Previous studies (Plum-
precipitation of soluble compounds (Randtke ; Ye
mer & Edzwald ; Huang et al. ) show that the
et al. ). Thus, the presence of NB in the M. aeruginosa
majority of THMFP comes from algal cells. Thus, a high
solution did not affect the coagulation-sedimentation per-
removal rate of total THMFP (91.8 ± 0.58%) was obtained.
formance directly.
Surprisingly, a high removal rate of THMFP in EOM (approximately 80%) was also obtained, which is much
Effect of the interaction of NB and M. aeruginosa on the
higher than the removal rate of DOC (31.6%). This phenom-
performance of coagulation-sedimentation
enon can be explained by the different removal efficiencies of dissolved organics by coagulation. It is reported that
The performance of coagulation-sedimentation in treating
coagulation can remove hydrophobic organics more effi-
NM5 and M. aeruginosa solution with three types of coagu-
ciently than hydrophilic organics, and the former contains
lant was studied, and the results at the coagulant dosages
considerably more THMFP than the latter (Edzwald ).
optimized for turbidity removal are shown in Figure 2. The
The specific ultraviolet absorbance (SUVA, the ratio of
specific coagulant type did not affect the coagulation-sedi-
UV254 to DOC) is regarded as an indicator of organic com-
mentation performance, and the removal rates of turbidity,
position, and a high value indicates that the water mainly
OD680, THMFP and MC-LR were similar for different
contains hydrophobic, aromatic and high molecular
coagulants at their optimized dosages (20 mg Al2O3/L for
weight compounds, which form THMs more easily during
aluminum sulfate, 44.5 mg Fe2O3/L for ferric chloride and
disinfection and can more easily be removed by coagulation
39 mg Al2O3/L for PAC). The removal rate of THMFP in
(Edzwald ). This value also decreased significantly after
EOM and residual turbidity in the NM5 settled water were
coagulation, from 2.69 to 1.73 L/mg/m. This change indi-
lower than in M. aeruginosa solution, while the removal
cated that the organic composition was greatly changed by
rates of OD680, total THMFP and intracellular MC-LR
coagulation with the more efficient removal of hydrophobic
were identical. The results of one-way analysis of variance
organics. Previous studies also indicated that proteins
(ANOVA) comparing the removal rates of THMFP in
account for 33% of the total DOC in the algal solution,
EOM and residual turbidity in the settled water for NM5
and can be removed completely by coagulation (Henderson
and M. aeruginosa solution supported this viewpoint
et al. ; Tsai et al. ). Proteins are also THMFPs,
(p ¼ 0.045 for turbidity and p ¼ 3.84 × 10–9 for THMFP).
according to the study by Scully et al. (). Thus, the
After sedimentation, more than 80% of the total THMFP
removal of proteins by coagulation may contribute to the
came from the EOM in the settled water of NM5, which
removal of THMFP in EOM. In the settled water, 70.3 ±
was higher than that observed in the M. aeruginosa solution
9.9% of the total THMFP came from the EOM, which was
(without NB). Obviously, the interaction between NB and
much higher than that before coagulation-sedimentation
M. aeruginosa changed the characteristics of the raw water
(less than 30%).
and affected the coagulation-sedimentation results.
Neither the performance of coagulation-sedimentation
The removal of NB by coagulation-sedimentation is
nor the coagulant dosage was affected by the addition of
shown in Figure 3. In general, coagulation-sedimentation
NB. The removal rates of all five parameters in NMf by
cannot remove NB efficiently, and the removal rates were
coagulation-sedimentation were approximately the same as
always less than 4%. The interaction between NB and M.
those in the M. aeruginosa solution.
aeruginosa did not affect the removal of NB by coagu-
It is predictable that NB does not affect the coagulation-
lation-sedimentation. However, there was a slightly higher
sedimentation of M. aeruginosa. NB is a weak hydrophobic
removal rate of NB in NMf than in NM5, although the differ-
material with a solubility of 2.1 g/L at 25 C (IPCS ),
ence was not statistically significant (one-way ANOVA,
and it cannot ionize in the water. These characteristics
p ¼ 0.065). The higher removal rate in NMf might be attrib-
imply that NB would not disturb coagulant hydrolysis or
uted to the adsorption of NB by M. aeruginosa during the
the coagulation process, including the charge neutralization
coagulation process.
W
62
Figure 2
Z. Liu et al.
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Effects of the interaction between M. aeruginosa and NB on coagulation
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Results of coagulation-sedimentation of M. aeruginosa solution and a mixture of NB and M. aeruginosa after a 5-day incubation (NM5). Coagulant: (a) Al2(SO4)3 20 mg Al2O3/L; (b) FeCl3 44.5 mg Fe2O3/L; (c) PAC 39 mg Al2O3/L.
Proposed mechanisms for the effects of the interaction on coagulation-sedimentation The present study showed that NB did not affect the performance of coagulation-sedimentation directly, and the interaction between NB and M. aeruginosa reduced the removal rate of THMFP in EOM and the residual turbidity in the settled water. These variations were independent of coagulant type. In fact, these differences were also observed in the pre-oxidation and coagulation-sedimentation experiments (Figure S4, supplementary data; available online at http://www.iwaponline.com/jws/ 063/081.pdf). The results indicated that the characteristics of Figure 3
|
Removal of NB by coagulation-sedimentation with three types of coagulants.
the raw water were changed by the interaction between NB
Coagulant dosage: Al2(SO4)3 20 mg Al2O3/L; FeCl3 44.5 mg Fe2O3/L; PAC 39 mg Al2O3/L. NM5 – a mixture of NB and M. aeruginosa after a 5-day incubation.
and M. aeruginosa, which affected the performance of coagu-
NMf – a fresh mixture of NB and M. aeruginosa without incubation.
lation-sedimentation.
ZP (mV)
initial NB concentration (160 μg/L), the growth of M. aeru-
lation-sedimentation (turbidity removal rate increased from less than 75% to more than 99%, and OD680 removal rate increased from less than 70% to more than 99%). After adjustment, the pH was similar in NM5 and the M. aeruginosa solution (9.34–9.76 for NM5 and 9.46–9.91 for M. aeruginosa). Thus, the initial difference in pH and alkalinity in the present study are negligible. Interaction with NB changed the surface charges of M. aeruginosa, which is responsible for the lower residual turbidity in the settled water. Zeta potential represents the potential stability of the colloidal system, and a weaker zeta potential promotes coagulation (Nachbaur et al. ; Sharp et al. ). The negative zeta potential in NM5
pH Extracellular
0.2729 ± 0.0152 37.20 ± 8.32
27.80 ± 6.51
0.0820 ± 0.0075
water, which greatly improved the performance of coagu-
0.0805 ± 0.0003
adjusted by Na2CO3 according to actual values in surface
37.96 ± 2.01
efficiency. However, in the present study, alkalinity was
37.35 ± 3.23
can affect the optimized coagulant dosage and the coagulant
In NM5
play significant roles in coagulation-sedimentation, which
In M. aeruginosa solution
out growth inhibition. Previous studies (Ye et al. ; Gottfried et al. ) have indicated that pH and alkalinity
Intracellular
resulting in a lower pH and higher alkalinity in NM5 with-
EOM
Kahara & Vermaat ). NB inhibited photosynthesis,
In the
alkalinity and cause an increase of pH (Talling ;
The total
cantly. Due to photosynthesis, phytoplankton can deplete
OD680 (cm 1)
affect the performance of coagulation-sedimentation signifi-
(NTU)
NB after a 5-day incubation, but these variations did not
Turbidity
The pH and alkalinity were changed by the presence of
MC-LR (μg/L)
parameters.
THMFP (μg/L)
M. aeruginosa were evident from differences in water quality
|
after a 5-day incubation. However, other effects of NB on
Table 1
were the same in NM5 and the M. aeruginosa solution
Comparison of water quality parameters in the M. aeruginosa solution and the mixture of NB and M. aeruginosa after a 5-day incubation (NM5)
ginosa was not inhibited by NB, and turbidity and OD680
40.36 ± 3.65
The water quality parameters of the M. aeruginosa solution and NM5 are shown in Table 1. With a non-lethal
51.16 ± 2.40
oxidized to form THMs during chlorination (Liu et al. ).
7.53–8.64
dissolved compounds, such as aniline, which can be further
8.76–9.33
dation, and the biodegradation process may produce
–
Alkalinity (mg
enhance the elimination of NB by adsorption and biodegra-
–
rate, among others (Liu et al. ). M. aeruginosa can
51.7 ± 6.4
UV254 (cm 1)
reducing the MC-LR productivity and the photosynthetic
CaCO3/L)
cell activities by enhancing the protein productivity and
68.4 ± 11.2
At a high concentration, NB can inhibit the growth of M. aeruginosa. Even at a low concentration, NB can affect
0.1381 ± 0.0132
Journal of Water Supply: Research and Technology—AQUA
796 ± 45
Effects of the interaction between M. aeruginosa and NB on coagulation
724 ± 72
|
2764 ± 88
Z. Liu et al.
2515 ± 112
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Effects of the interaction between M. aeruginosa and NB on coagulation
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increased and therefore enhanced the removal of turbidity
The results indicated that coagulation-sedimentation can
by coagulation-sedimentation. Takaara et al. () report
significantly improve the quality of water containing
that M. aeruginosa cells can secrete negatively charged
M. aeruginosa. Although NB did not affect the coagu-
hydrophilic substances, which can decrease zeta potential
lation-sedimentation process directly, the presence of NB
and inhibit their coagulation. The presence of NB may inhi-
did change the performance of coagulation-sedimentation
bit the secretion of these compounds by M. aeruginosa,
after a 5-day incubation with M. aeruginosa, including a
which would result in increased zeta potential.
reduced removal rate of THMFP in EOM and a lower
NB-enhanced production of THMFP in M. aeruginosa
residual turbidity in the settled water. These effects resulted
EOM may have led to the low removal rate of THMFP in
from the interaction between NB and M. aeruginosa. The
NM5. Our previous study (Liu et al. ) indicates that
weak zeta potentials caused by the interaction and the
THMFP productivity in EOM can increase up to 50% in
degradation products of NB were responsible for these
the presence of NB, although NB cannot be chlorinated to
variations.
form THMs directly. These increased THMFP values come
The present results imply that the interaction between
from the proteins secreted by M. aeruginosa and the degra-
xenobiotics and algae on water treatment processes should
dation products of NB. Figure 1 shows a high removal rate
be considered when combined polluted water is used as
of THMFP in EOM by coagulation, which implies that
the drinking water source. However, due to the complexity
most of the THMFP secreted by M. aeruginosa can be
of xenobiotics and the diversity of algae and cyanobacteria,
removed by coagulation-sedimentation. Thus, the increased
the present study cannot represent the whole scenario, and
protein content would not affect the removal of THMFP sig-
further study is necessary.
nificantly. However, the soluble degradation products of NB cannot be removed efficiently by coagulation-sedimentation, which caused a lower THMFP removal rate than without
ACKNOWLEDGEMENTS
NB and resulted in a higher proportion of THMFP in the EOM of the settled water (more than 80%, compared with
This work was supported by the Funds for Creative
70.3% without NB). These products increased the initial
Research Groups of China (Grant No. 51121062) and the
value of UV254 and resulted in a higher residual THMFP
National Natural Science Foundation of China (Number
concentration in the EOM after coagulation (228 ± 13 μg/
50778048).
L), compared with the M. aeruginosa solution without NB (142 ± 12 μg/L). The interaction between NB and M. aeruginosa increased the disinfection risk significantly over the
REFERENCES
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it
did
negatively
affect
the
performance
of
coagulation-sedimentation. This effect should be considered when water containing NB and M. aeruginosa is used as drinking water resource.
CONCLUSIONS In the present study, the impacts of the interaction between NB and M. aeruginosa on the performance of coagulationsedimentation were studied by using a bench-scale jar test.
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silicate cement suspensions during early age hydration. J. Colloid Interface Sci. 202 (2), 261–268. Plummer, J. D. & Edzwald, J. K. Effect of ozone on algae as precursors for trihalomethane and haloacetic acid production. Environ. Sci. Technol. 35 (18), 3661–3668. Randtke, S. J. Organic contaminant removal by coagulation and related process combinations. J. Am. Water Works Assoc. 80 (5), 40–56. Scully Jr., F. E., Howell, G. D., Kravitz, R. & Jewell, J. T. Proteins in natural waters and their relation to the formation of chlorinated organics during water disinfection. Environ. Sci. Technol. 22 (5), 537–542. Semple, K. T. & Cain, R. B. Biodegradation of phenols by the alga Ochromonas danica. Appl. Environ. Microbiol. 62 (4), 1265–1273. Semple, K. T., Cain, R. B. & Schmidt, S. Biodegradation of aromatic compounds by microalgae. FEMS Microbiol. Lett. 170, 291–300. Sharp, E. L., Jarvis, P., Parsons, S. A. & Jefferson, B. The impact of zeta potential on the physical properties of ferricNOM flocs. Environ. Sci. Technol. 40 (12), 3934–3940. Shen, Q., Zhu, J., Cheng, L., Zhang, J., Zhang, Z. & Xu, X. Enhanced algae removal by drinking water treatment of chlorination coupled with coagulation. Desalination 271 (1–3), 236–240. Takaara, T., Sano, D., Masago, Y. & Omura, T. Surface-retained organic matter of Microcystis aeruginosa inhibiting coagulation with polyaluminum chloride in drinking water treatment. Water Res. 44 (13), 3781–3786. Talling, J. F. The depletion of carbon dioxide from lake water by phytoplankton. J. Ecol. 64 (1), 79–121. Tian, J., Chen, Z., Nan, J., Liang, H. & Li, G. Integrative membrane coagulation adsorption bioreactor (MCABR) for enhanced organic matter removal in drinking water treatment. J. Membr. Sci. 352 (1–2), 205–212. Tsai, B.-N., Chang, C.-H. & Lee, D.-J. Fraction of soluble microbial products (SMP) and soluble extracellular polymeric substances (eps) from wastewater sludge. Environ. Technol. 29 (10), 1127–1138. Tukaj, Z. The effect of fuel oil on the ultrastructure of the chlorococcal alga Scenedesmus armatus. Protoplasma 151 (1), 47–56. Ye, C., Wang, D., Shi, B., Yu, J., Qu, J., Edwards, M. & Tang, H. Alkalinity effect of coagulation with polyaluminum chlorides: role of electrostatic patch. Colloids Surf. A Physicochem. Eng. Asp. 294 (1–3), 163–173. Zamyadi, A., MacLeod, S. L., Fan, Y., McQuaid, N., Dorner, S., Sauvé, S. & Prévost, M. Toxic cyanobacterial breakthrough and accumulation in a drinking water plant: a monitoring and treatment challenge. Water Res. 46 (5), 1511–1523.
First received 26 April 2013; accepted in revised form 20 September 2013. Available online 31 October 2013
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Biosorption studies for the removal of ferrous ion from aqueous solution by Aspergillus terreus and Trichoderma viride: kinetic, thermodynamic and isothermal parameters Sarafadeen Olateju Kareem, Abideen Idowu Adeogun and S. O. Omeike
ABSTRACT Environmental implications and the tendency of heavy metals to accumulate in selected tissues of plants and animals, as well as their overall potential to be toxic even at relatively minor levels of exposure, are a source of concern. The use of cheap and effective biological means for heavy metal remediation has been advocated. This study examines the biosorption and bioaccumulation of ferrous ion by Aspergillus terreus (A. terreus) and Trichoderma viride (T. viride) in a batch system. The effects of some important parameters, such as initial metal concentration, temperature and inoculum concentration on biosorption capacity were examined. Langmuir, Freudlinch, Temkin and Dubinin–Radushkevich models were applied to explain the biosorption isotherms of Fe(II) onto the
Sarafadeen Olateju Kareem S. O. Omeike Department of Microbiology, Federal University of Agriculture, Abeokuta, Nigeria Abideen Idowu Adeogun (corresponding author) Department of Chemistry, Federal University of Agriculture, Abeokuta, Nigeria E-mail: abuaisha2k3@yahoo.com
biosorbents. The process fitted well into pseudo first order kinetic model and was best explained by the Langmuir isotherm with maximum absorption capacity of 6.33 and 7.50 mg/g for A. terreus and T. viride, respectively. The calculated thermodynamic parameters (ΔG , ΔH and ΔS ) showed that the W
W
W
biosorption of the ferrous ion to the organisms is feasible, spontaneous and exothermic in nature at low temperature. Key words
| Aspergillus terreus, biosorption, kinetics and isotherms, Trichoderma viride
INTRODUCTION The presence of heavy metal ions in the environment is a
in Fenton reactions leading to the production of high levels
major concern due to their toxicity to many life forms.
of toxic hydroxyl radicals (·OH) and other reactive oxygen
Industrial processes, such as mining operations, sludge dis-
species (H2O2, O2 ) (Bode et al. ; Thongbai & Good-
posal, metal as plating and the manufacture of electrical
man ). These compounds react with polyunsaturated
equipment lead to the release of metal ions into the environ-
fatty acids, protein and nucleic acids, thus giving rise to
ment and, invariably, they become pollutants in the
the
environment. The toxic nature of these pollutants has
(Alscher et al. ). Serious toxicity is likely with ingestion
caused increased concern regarding their removal from
of more than 60 mg/kg. Toxic effects of iron may occur at
industrial effluents (Senthilkumar et al. ). Heavy
doses of 10–20 mg/kg of elemental iron (Rao & Georgieff
metals are not biodegradable and tend to accumulate in
). When high concentrations (over 200 ppm) of iron
living organisms, causing various diseases and disorders
are absorbed, for example by haemochromatosis patients,
(Manaham ; Yu ).
iron is stored in the pancreas, the liver, the spleen and
destruction
of
numerous
endocellular
structures
Although iron is an essential element for life, its excess
the heart and may damage these vital organs. Thus, the
in plant and animal tissues may be responsible for a wide
need for the removal of ferrous ion from wastewater
range of metabolic disorders, due mainly to its involvement
is justified.
doi: 10.2166/aqua.2013.109
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Removal of Fe(II) from aqueous solution by A. terreus and T. viride
Iron removal from water is mostly carried out in drinking water preparation, because mineral water contains high
Journal of Water Supply: Research and Technology—AQUA
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mass (Hemambika et al. ). One mL of deionized water was added to the dried spores as necessary.
amounts of iron ions. These influence water color, odor and turbidity. In wastewater treatment, iron removal may be
Preparation of aqueous solution of metal ions
achieved by cumbersome and high-cost processes which justify alternative technology. Biosorption of heavy metals by
The aqueous solutions of ferrous ion were prepared freshly
microbial cells has been recognized as a potential alterna-
as necessary from analytical grades of Fe2SO4.H2O
tive to existing technologies for recovery of heavy metals
(Sigma, USA). One thousand mg/L aqueous solution
from industrial waste streams. Most studies of biosorption
(stock solution) of this salt was prepared with deionized
for metal removal have involved the use of either labora-
water in 1% HNO3 solution and the stock solution was
tory-grown microorganisms or biomass generated by the
diluted with deionized water to obtain the working standard
pharmacology and food processing industries or wastewater
solutions. The pH adjustments of the solutions were made
treatment units (Tsezos & Velosky ; Townsley et al.
with aliquots of 1.0 mol/L of HCl and NaOH. The pH of
; de Rome & Gadd ; Macaskie ; Costa &
the solution was checked on an electronic pH meter
Leite ; Rao et al. ; Dias et al. ). Many aquatic
(Thermo Russell, USA), which had earlier been standar-
microorganisms, such as fungi, bacteria, yeast and algae
dized with standard buffer solution.
can take up dissolved metals from their surroundings onto their bodies and can be used for removing heavy metal
Equilibrium studies
ions successfully (Aksu et al. ). In this study, Aspergillus terreus (A. terreus) and Trichoderma viride (T. viride) were
Equilibrium adsorption isotherms were performed in a
used as effective and low-cost sorbents for the removal of
batch process as previously described (Bello et al. ;
ferrous ion from aqueous solution. The effects of initial
Adeogun et al. , ). The amount of metal ion adsorbed
metal concentration, pH, temperature and biosorbent dose
by the biosorbent at equilibrium, Qe (mg/g), was calculated
were also studied. The equilibrium data were analyzed
using Equation (1):
with Langmuir, Freundlich, Redlich–Peterson and Dubinin– Radushkevich (D–R) isotherms. The thermodynamic parameters
were
also
elucidated
from
the
temperature
Qe ¼
(Co Ce )V , W
(1)
dependent of the biosorption process. where Co and Ce (mg/L) are the liquid-phase concentrations of the metal ion at initial and equilibrium, respectively. V is the volume of the solution (L), and W is the mass of dry
MATERIALS AND METHODS
adsorbent used (g).
Biosorbent preparation
Bioaccumulation studies
Metal-degrading fungal strains of A. terreus and T. viride iso-
The procedure was similar to that of equilibrium studies,
lated from contaminated soil were collected from the
except that samples were prepared and withdrawn at an
Microbiology Department of the Federal University of Agri-
interval of 24 hours for the determination of residual iron
culture Abeokuta, southwestern Nigeria. The biomass was
in the solution. The amount of iron absorbed at intervals
suspended in 10 mL deionized water and centrifuged at
was expressed as a percentage:
4,000 rpm for 10 min to separate vegetative materials from spores. The supernatant was decanted and the precipitated spores were dried in a hot air-oven and weighed to constant
Q% ¼
(Co Ce )V × 100 W
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Removal of Fe(II) from aqueous solution by A. terreus and T. viride
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). Optimum iron sorption at pH 6 and 7 was observed
Batch kinetic studies
for A. terreus and T. viride, respectively (Figure 1). This indiThe procedures for kinetic experiments were basically iden-
cates the presence of weakly positive to negative ions on the
tical to those of equilibrium tests. The aqueous samples were
surface of the biomass to interact with ferrous ion present in
taken at pre-set time intervals, and the concentrations of the
the solution and form bonds, binding the metals to the bio-
metal ions were similarly determined. The amount of metal
mass surface (Faria et al. ). At high pH, there is an
ion adsorbed at time t, Qt (mg/g), was calculated using
abundance of negatively charged ions on the surface of the
Equation (2):
biomass and this will attract more positively charged metal ion to the surface for binding.
Qt ¼
(Co Ce )V W
(2)
where Co and Ct (mg/L) are the liquid-phase concentrations
Effect of biosorbent dosage The effect of biosorbent dosages on the removal of Fe(II) ion
of the metal ion at initial and at time t, respectively. V is the
from aqueous solution is presented in Figure 2. The highest
volume of the solution (L), and W is the mass of dry adsor-
metal concentration was obtained at the dosage of 1.6 mg of
bent used (g).
the biosorbents. Although at lower dosage T. viride remove more of the metal ion than A. terreus, as the dosage increases the capacity for the removal of the metal ion increases to the maximum of about 89% at 1.6 mg dosage
RESULTS AND DISCUSSION
for the two biosorbents. As the biosorbent dosage increases above optimum dosage values, a decrease in the percentage
Effect of hydrogen ion concentration
of metallic ions removal was observed. This may be attributed to the concentration gradient between adsorbate and
pH is described as the most important factor for ion uptake
biosorbent with increasing biomass concentration causing
(Geddie & Sutherland ). It strongly influences the spe-
a decrease in the amount of metallic ion adsorbed per
ciation and biosorption availability of the metal ions
gram of biomass (Vaghetti et al. ).
(Esposito et al. ), alters activity of binding sites and also affects the types of ion in the solution (Adeogun et al.
Figure 1
|
Effect of pH on sorption capacities of A. terreus and T. viride.
Figure 2
|
Effect of biosorbent dosage on sorption capacities of A. terreus and T. viride.
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Effect of temperature Optimization parameters for iron removal showed an optiW
mum uptake at a temperature of 30 C (Figure 3), with reduced uptake above and below this temperature indicating that sorption occurs best at the growth temperature of sorbents. This conforms with several studies which state that temperature has less influence on sorption performances in W
the range of 20–35 C, and its overall effect is minimal because sorption takes place over a narrow temperature range of 10– 70 2035 C (Aksu et al. ; Vegliò & Beolchini ). W
Effect of contact time and initial metal concentration Figures 4 and 5 illustrate the effect of contact time on Fe(II) ion biosorption by T. viride and A. terreus, respectively.
Figure 4
|
The effect of contact time on Fe(II) ion biosorption by T. viride.
Figure 5
|
The effect of contact time on Fe(II) ion biosorption by A. terreus.
From the figures, it can be seen that the equilibrium time for metal ion biosorption T. viride is concentration dependent while that of A. terreus does not depend on initial metal ion concentration. This is as a result of the high affinity of A. terreus for metal ion (Dias et al. ). Biosorption kinetics Pseudo first order kinetics The study of adsorption kinetics is important in the treatment of aqueous effluents as it provides valuable information on
the reaction pathways and the mechanism of the adsorption process. Many kinetic models have been developed in order to find intrinsic kinetic adsorption constants; traditionally, the kinetics of metal ions adsorption is described following the expressions originally given by Largegren (). A simple kinetic analysis of adsorption under the pseudo first order assumption is given by Equation (3) below:
Figure 3
|
Effect of temperature on sorption capacities of A. terreus and T. viride.
dQt ¼ k1 (Qe Qt ) dt
(3)
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Removal of Fe(II) from aqueous solution by A. terreus and T. viride
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where Qe and Qt are the amounts of the metal ion biosorbed
where k2 (g mg 1 min 1) is the rate constant of second order
(mg g 1) at equilibrium and at time t (min), respectively, k1 is
adsorption. The parameters for pseudo second order theor-
1
the rate constant of biosorption (min ) and t is the contact
etical fitting of time-dependent biosorption of the metal
time (min). The integration of Equation (3) with initial con-
ion onto the biosorbent (Qt) are presented in Table 1. The
ditions, Qt ¼ 0 at t ¼ 0 and Qt ¼ Qt at t ¼ t, yields Equation (4):
correlation coefficients for the second order kinetic model ranged between 0.986 and 0.989 indicating the suitability
Qt ¼ Qe (1 e k1 t )
(4)
of the pseudo first order kinetics over that of the second order kinetic equation model.
The kinetic data were analyzed with non-linear regression analysis method using a program written on MicroMath Scientist software (Salt Lake City, USA). The parameters
Statistical test for the kinetic data
used for fitting the pseudo first order kinetics are shown in
Although the R 2, i.e., the correlation coefficients used to
Table 1. The correlation coefficient values of 0.996 and the
compare the data, the pseudo first and second order kinetic
experimental Qe values are not far from the calculated ones.
function which measures the differences (% SSE) in the
Pseudo second order kinetics
amount of the metallic metal ion uptaken by the adsorbent
A second order kinetic model which is based on equilibrium adsorption (Malik ) was used to compare the Qe values with that of pseudo first order rate model. It is expressed as shown by Equation (5): dQt ¼ k2 (Qe Qt )2 dt
(5)
Upon integration and rearrangement, the second order rate equation becomes Equation (6): Qt ¼
|
predicted by the models, (Qcal), and the actual, i.e., Qexp measured experimentally (Vaghetti et al. ; Adeogun et al. ). The validity of each model was determined by the sum of error squares (SSE, %) given by Equation (7): sffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi (q( exp ) q(cal) )2 %SSE ¼ N
where N is the number of data points. The higher the value of R 2 and the lower the value of SSE, the better will be the
(6)
the first order model confirm the acceptability of the model over the second order model.
Kinetic parameters for the biosorption of Fe(II) by A. terreus and T. viride Pseudo first order Co (mg L 1)
A. terreus
T. viride
(7)
goodness of fit. From Table 1, the lower values of % SSE for
k2 Q2e t
1 þ k2 Qe t
Table 1
models were also evaluated further by the percentage error
50
Ce (mg L 1)
2.37
Pseudo second order
Qe (exp) (mg g 1)
Qe(cal) (mg g 1)
k1 (h 1)
R2
% SSE
Qe
k2 (g mg h 1)
R2
% SSE
2.977
3.112
0.113
0.996
0.015
3.867
0.028
0.989
0.099
(calc)
100
9.84
5.635
5.891
0.113
0.996
0.028
7.319
0.015
0.989
0.187
125
22.89
6.382
6.672
0.113
0.996
0.032
8.289
0.013
0.989
0.212
150
61.74
5.516
5.767
0.113
0.996
0.028
7.165
0.015
0.989
0.183
200
103.11
6.056
6.331
0.113
0.996
0.031
7.865
0.014
0.989
0.201
50
1.33
3.042
3.180
0.113
0.996
0.015
3.951
0.027
0.986
0.101
100
6.03
5.873
6.140
0.113
0.996
0.030
7.628
0.014
0.986
0.195
125
14.88
6.883
7.195
0.113
0.996
0.035
8.940
0.012
0.989
0.229
150
37.55
7.028
7.347
0.113
0.996
0.035
9.129
0.012
0.986
0.233
200
83.79
7.263
7.593
0.113
0.996
0.037
9.434
0.011
0.989
0.241
10.63 0.978 4.42 6.91 0.999 1.033 0.423 3.607 0.986 6.413 3.945 0.009 0.996 0.549
0.970 9.18
7.505
aRP KRP RL
KF ((mg g 1) (L g 1))1/n
T. viride
Table 2
R2
Biosorption isotherms for Fe(II) biosorption on T. viride.
b (L mg 1)
|
Qo (mg g 1)
Figure 7
Freundlich
Biosorption isotherms for Fe(II) biosorption on A. terreus.
Langmuir
|
|
Figure 6
Isotherm parameters for the biosorption of Fe(II) by A. terreus and T. viride
n
R2
Redlich–Peterson
β
R2
Figures 6 and 7 are shown in Table 2.
5.99
USA). The parameters obtained for the isotherm models in
0.997
Dubinin
written on MicroMath Scientist software (Salt Lake City,
1.138
the non-linear regression analysis method using a program
0.163
to describe the equilibrium data. Data were analyzed with
1.830
β × 107 mol2 J 2
Freundlich, D–R and Redlich–Peterson models were used
Qm (mg g 1)
equilibrium relationships. In the present study, Langmuir,
0.978
R2
phase and that on the adsorbent’s surface at a given condition. Several isotherms have been developed to describe
8.183
ship between the adsorbate concentration in the liquid
3.636
An adsorption isotherm represents the equilibrium relation-
0.011
Ea (kJ mol 1)
Adsorption isotherms
7.38
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0.927
Removal of Fe(II) from aqueous solution by A. terreus and T. viride
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where KF is the Freundlich constant related to sorption
Langmuir isotherm model
capacity ((mg g 1) (L g 1))1/n and n is related to the adsorpLangmuir, in 1918, observed sorption phenomena and
tion intensity of the adsorbent. The value of KF from this
suggested that uptake occurs on a homogeneous surface
study showed that biosorbents have similar affinity for the
by
metal ion. The value of 1/n showed that the surfaces are het-
monolayer
sorption
without
interaction
between
adsorbed molecules. He proposed the sorption isotherm
erogeneous (Krobba et al. ).
based on the assumptions that: (i) adsorbates are chemically adsorbed at a fixed number of well-defined sites; (ii) each
Redlich–Peterson isotherm
site can only hold one adsorbate species; (iii) all sites are energetically equivalent; and (iv) that there are no inter-
A three parameter Redlich–Peterson equation has been pro-
actions between the adsorbate species.
posed to improve the fit by the Langmuir or Freundlich
The Langmuir isotherm equation is written as Equation (8): qe ¼
Qmax bCe 1 þ bCe
(8)
where Ce is the supernatant concentration after the equilibrium of the system (mg L 1), b the Langmuir affinity constant (L mg 1) and Qmax is the maximum adsorption capacity of the material (mg g 1) assuming a monolayer of adsorbate uptaken
equation and is given by Equation (11): Qeq ¼
KRP Ce 1 þ aRP Ceβ
(11)
where KR, bR and β are the Redlich–Peterson parameters, β lies between 0 and 1 (Vaghetti et al. ). For β ¼ 1, Equation (11) converts to the Langmuir form. The adsorption model constants are presented in Table 2 and the isotherms are shown in Figures 5 and 6. The value of β
by the adsorbent. The values of R 2 in Table 2 for the Langmuir isotherm showed better fittings (Figures 6 and 7) for the metal ions
obtained in this study shows that the model operates closely to the Langmuir isotherm.
by the two biosorbents. Separation factor (RL) is defined by the relationship in Equation (9) (Anirudhan & Radhak-
D–R isotherm
rishnan ): RL ¼ 1=(1 þ bCi )
(9)
The D–R model (Dubinin et al. ) was chosen to estimate the heterogeneity of the surface energies and also to deter-
where Ci is the initial concentration (mg L ). The value of
mine the nature of biosorption processes as physical or
the separation parameter provides important information
chemical. The D–R sorption isotherm is more general than
about the nature of adsorption. If RL value of zero implies
the Langmuir isotherm as its derivation is not based on
1
irreversible adsorption, it is a favorable process when 0 < RL < 1, linear when RL is 1 or unfavorable when RL is greater than 1 (Chen et al. ). The values of RL in this study and presented in Table 2 implied that the process is favorable.
Freundlich isotherm model The Freundlich isotherm is based on the assumption of nonideal adsorption on heterogeneous surfaces and the linear form of the isotherm can be represented as in Equation (10) (Freundlich ): Qt ¼ KF Ce1=n
(10)
Figure 8
|
Thermodynamic plot for Fe(II) biosorption on A. terreus and T. viride.
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Table 3
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Thermodynamic parameters for the biosorption of Fe(II) by A. terreus and T. viride A. terreus
T. viride
Temperature (K)
ΔG (kJ mol 1)
ΔS (kJ mol 1 K 1)
ΔH (kJ mol 1)
R2
ΔG (kJ mol 1)
ΔS (kJ mol 1 K 1)
ΔH (kJ mol 1)
R2
308
4.00
0.138
60.43
0.99
4.23
0.279
90.52
0.95
318
2.21
2.18
323
1.24
0.15
ideal assumptions such as, equipotent of the sorption sites,
used to estimate the thermodynamic parameters owing to
absence of hindrance between sorbed and incoming par-
its
ticles and surface homogeneity on microscopic level
(Nkiko et al. ). A plot of ΔG against the temperature
(Weber & Morris ; Malik ). The D–R isotherm is
(Figure 8) gives a straight line graph with intercept as ΔH
represented by Equation (12):
and slope as ΔS . The thermodynamic parameters are pre-
temperature
dependence
as
previously
explained
W
W
W
sented in Table 3. The negative values of ΔG free energy W
Qt ¼ Qm e
βε2
(12)
where Qm is the theoretical saturation capacity (mol g 1), β
change of the process implies a thermodynamically feasible and spontaneous biosorption process.
is a constant related to the mean free energy of adsorption per mole of the adsorbate (mol2 J 2) and ε is the polanyi potential given by the relation ε ¼ RT ln(1 þ 1/Ce). Ce is the equilibrium concentration of adsorbate in solution (mol L 1), R (J mol 1 K 1) is the gas constant and T (K) is the absolute temperature. The constant β gives an idea about the mean free energy E (kJ/mol) of adsorption per molecule of the adsorbate when it is transferred to the surface of the solid from infinity in the solution and can be
CONCLUSION Results of this study showed that iron could be effectively removed from solution by low amounts of A. terreus and T. viride biomass in solution. The biosorption capacity values of 6.33 and 7.51 mg/g for A. terreus and T. viride, respectively, in this study compared favorably with those
calculated from the relationship (Kundu & Gupta ):
reported in the literature. Sag et al. () reported a value
pffiffiffiffiffiffiffiffiffi E ¼ 1= 2β
() reported a value of 6.04 mg/g using dried sludge for
(13)
If the magnitude of E is between 8 and 16 kJ mol 1, the sorption process is supposed to proceed via chemisorption, while for values of E < 8 kJ mol 1, the sorption process is
of 5.1 mg/g using Rhizopus arrhizus while Shokoohi et al. iron removal. High uptake of iron even at a concentration of 250 mg/L shows that suspension or trapping of the spore mass on suitable matrices will further enhance their sorption capabilities and its scaling-up for use in effluent clean-up, while the Langmuir and Freundlich models further
physical in nature. Since the values obtained in this study
confirm the high sorption property of these biomasses. A.
are within the ranges specified by the model, the process
terreus and T. viride biomass can be effectively used as
therefore, is purely chemisorption.
material for biological removal of iron from aqueous solution over a wide range of concentration and pH.
Biosorption thermodynamics
REFERENCES Distribution of the metal ion between the solution and the biosorbent is an equilibrium process associated with the equilibrium constant, KD. The equilibrium constant was
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(Spondias mombin): kinetics and equilibrium studies. Pakistan J. Sci. Ind. Res. 53, 246–251. Adeogun, A. I., Ofudje, A. E., Idowu, M. A. & Kareem, S. O. Equilibrium, kinetic, and thermodynamic studies of the biosorption of Mn(II) ions from aqueous solution by raw and acid-treated corncob biomass. BioResources 6, 4117–4134. Adeogun, A. I., Kareem, S. O., Durosanya, J. B. & Balogun, S. E. Kinetics and equilibrium parameters of biosorption and bioaccumulation of lead ions from aqueous solutions by Trichoderma longibrachiatum. J. Microbiol. Biotechnol. Food Sci. 1, 1221–1234. Aksu, Z., Sag, Y. & Kutsal, T. The biosorption of copper (II) by C. vulgaris and Z. ramigera. Environ. Technol. 13, 579–586. Alscher, R. G., Donahue, J. L. & Cramer, C. L. Reactive oxygen species and antioxidants: relationships in green cells. Physiol. Plantarum 100, 224–233. Anirudhan, T. S. & Radhakrishnan, P. G. Thermodynamics and kinetics of adsorption of Cu(II) from aqueous solutions onto a new cation exchanger derived from tamarind fruit shell. J. Chem. Thermodynam. 40, 702–709. Bello, O. S., Adeogun, A. I., Ajaelu, J. C. & Fehintola, E. O. Adsorption of methylene blue onto activated carbon derived from periwinkle shells: kinetics and equilibrium studies. Chem. Ecol. 24, 285–295. Bode, K., Döring, O., Luthje, S., Neue, H. U. & Böttger, M. The role of active oxygen in iron tolerance of rice (Oryza sativa L.). Protoplasma 184, 249–255. Chen, Z., Ma, M. & Han, M. Biosorption of nickel and copper onto treated alga (Undaria pinnatifida): Application of isotherm and kinetic models. J. Hazard. Mater. 155, 327–333. Costa, A. C. A. & Leite, S. G. C. Metal biosorption by sodium alginate immobilized Chlorella homosphaera cells. Biotechnol. Lett. 13, 559–562. de Rome, L. & Gadd, G. M. Copper adsorption by Rhizopus arrhizus, Cladosporium resinae and Penicillium italicum. Appl. Microbiol. Biotech. 26, 84–90. Dias, M. A., Lacerda, I. C. A., Pimentel, P. F., de Castro, H. F. & Rosa, C. A. Removal of heavy metals by an Aspergillus terreus strain immobilized in a polyurethane matrix. Lett. Appl. Microbiol. 34, 46–50. Dubinin, M. M., Zaverina, E. D. & Radushkevich, L. V. Sorption and structure of active carbons. I. Adsorption of organic vapors. Zhurnal Fizicheskoi Khimii 21, 1351–1362. Esposito, A., Pagnanelli, F. & Vegliò, F. pH-related equilibria models for biosorption in single metal systems. J. Chem. Eng. Sci. 57, 307–313. Faria, P. C. C., Orfao, J. J. M. & Pereira, M. F. R. Adsorption of anionic and cationic dyes on activated carbons with different surface chemistries. Water Res. 38 (8), 2043–2052. Freundlich, H. M. F. Over the adsorption in solution. J. Phys. Chem. 57, 385–471. Geddie, J. L. & Sutherland, I. W. Uptake of metals by bacterial polysaccharides. J. Appl. Microbiol. 74, 467–472. Hemambika, B., Johncy Rani, M., Hemapriya, J. & Rajesh Kannan, V. Comparative assessment of heavy metal removal by
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immobilized and dead bacterial cells: a biosorption approach. Afr. J. Environ. Sci. Technol. 4 (2), 077–083. Krobba, A., Nibou, D., Amokrane, S. & Mekatel, H. Adsorption of copper (II) onto molecular sieves NaY. Desal. Water Treat. 37, 31–37. Kundu, S. & Gupta, A. K. Arsenic adsorption onto iron oxide-coated cement (IOCC): regression analysis of equilibrium data with several isotherm models and their optimization. Chem. Eng. J. 122 (1–2), 93–106. Largegren, S. About the theory of so-called adsorption of soluble substances. Kungliga Suensk Vetenskapsakademiens Handlingar 241, 1–39. Macaskie, L. E. An immobilized cell bioprocess for the removal of heavy metals from aqueous flows. J. Chem. Tech. Biotechnol. 49, 357–379. Malik, P. K. Dye removal from wastewater using activated carbon developed from sawdust: adsorption equilibrium and kinetics. J. Hazard. Mater. B113, 81–88. Manaham, S. E. Environmental Chemistry, 7th edn. CRC Press, Boca Raton, FL. Nkiko, M. O., Adeogun, A. I., Babarinde, N. A. A. & Sharaibi, O. J. Isothermal, kinetics and thermodynamics studies of the biosorption of Pb(II) ion from aqueous solution using the scale of croaker fish (Genyonemus lineatus). J. Water Reuse Desal. 3, 239–248. Rao, C. R. N., Iyengar, L. & Venkobachar, C. Sorption of copper (II) from aqueous phase by waste biomass. J. Environ. Eng. Div. ASCE 119, 369–377. Rao, R. & Georgieff, M. K. Iron therapy for preterm infants. Clin. Perinatol. 36 (1), 27–42. Sag, Y., Yalçuk, A. & Kutsal, T. Full competitive biosorption of chromium (VI) and iron (III) ions from binary metal mixtures by Rhizopus arrhizus: Use of competitive Langmuir model. Process Biochem. 31, 573–585. Shokoohi, R., Saghi, M. H., Ghafari, H. R. & Hadi, M. Biosorption of iron from aqueous solution by dried biomass of activated sludge. Iran J. Environ. Health Sci. Eng. 6 (2), 107–114. Senthilkumar, S., Bharathi, S. & Nithyanandhi, S. Biosorption of toxic heavy metals from aqueous solution. Bioresour. Technol. 75, 163–165. Thongbai, P. & Goodman, B. A. Free radical generation and postanoxic injury in rice grown in an iron-toxic soil. J. Plant Nutr. 23, 1887–1900. Townsley, C. C., Ross, I. S. & Atkins, A. S. Biorecovery of metallic residues from various industrial effluents using filamentous fungi. In: Fundamental and Applied Biohydrometallurgy (R. W. Lawrence, R. M. R. Branion & H. G. Ebner, eds). Elsevier, Amsterdam, The Netherlands, pp. 279–289. Tsezos, M. & Velosky, B. The mechanism of uranium biosorption by Rhizopus arrhizus. Biotechnol. Bioeng. 29, 385–401. Vaghetti, J. C. P., Lima, E. C., Royer, B., da Cunha, B. M., Cardoso, N. F., Brasil, J. L. & Dias, S. L. P. Pecan nutshell as
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biosorbent to remove Cu(II), Mn(II) and Pb(II) from aqueous solution. J. Hazard. Mater. 162, 270–280. Veglio, F. & Beolchini, F. Removal of metals by biosorption: a review. Hydrometallurgy 44 (3), 301–316.
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Weber, W. J. & Morris, J. C. Kinetics of adsorption on carbon from solution. J. Sanitation Eng. Div. ASCE 89, 31–60. Yu, M. H. Environmental Toxicology – Biological and Health Effects of Pollutants, 2nd edn. CRC Press, Boca Raton, FL.
First received 4 June 2013; accepted in revised form 26 September 2013. Available online 15 November 2013
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Assessment of water qualities and evidence of seawater intrusion in a deep confined aquifer: case of the coastal Djeffara aquifer (Southern Tunisia) Adel Kharroubi, Soumaya Farhat, Belgacem Agoubi and Zouhir Lakhbir
ABSTRACT Geochemical analyses of groundwater samples from the Djeffara confined aquifer (Southern Tunisia) were performed. The distribution of saline waters was investigated to identify the origin of the groundwater contamination. The aquifer was shown to be affected by an abnormal increase in groundwater salinity. Near the recharge zone, the groundwater salinity does not exceed 2.5 g l 1 but reaches 7 g l 1 in the northeast of the study area. Due to over pumping, groundwater level decline is so important that it disturbs the equilibrium between fresh and saline waters. The salinity distribution coupled with the structure and geology of the Djeffara aquifer suggest current seawater intrusion is possible through the deep fault systems affecting the zone. The groundwater level was shown to be highly correlated with the sea level fluctuation in the area near the fault systems, suggesting a communication between the sea and the confined aquifer. Groundwater salinization is probably
Adel Kharroubi Soumaya Farhat Belgacem Agoubi (corresponding author) Higher Institute of Water Sciences and Techniques, University of Gabes, Tunisia, Cité Erryadh 6072, Gabes, Tunisia E-mail: Belgacem.Agoubi@isstegb.rnu.tn Zouhir Lakhbir Société Nationale d’Exploitation et de Distribution d’Eau (SONEDE), Direction Production, Jerba, Tunisia
related to infiltration of seawater through the faults. However, an intrusion on the side of the discharge area of the aquifer may also be possible. The bromide and chlorine analyses coupled with the SO4/Cl ratio confirmed that the mixing between fresh and saline waters is the main origin of groundwater salinization. Key words
| aquifer, fault systems, groundwater, seawater intrusion
INTRODUCTION In arid and semi-arid regions, groundwater is the main
Kouzana et al. ; Martos et al. ). The mixing between
source of fresh water. It is required for drinking purposes,
groundwater and seawater can be diagnosed using many
tourism and agricultural activities. The increasing demands
techniques such as geochemical analyses, minor elements
for fresh water lead to groundwater pumping intensification.
and isotopic tracers. In many cases, tracers like Sr and Br
High pumping rates cause groundwater levels to decline and
can be used to identify the origin of groundwater saliniza-
therefore change the flow direction, which comes from the
tion when a single process occurs (Boluda-Botella et al.
sea towards the aquifer. When demanding groundwater
; Kim et al. ). Cl /Br and I /Cl ratios and spatial
withdrawals from aquifers exceed the recharge rate, sea-
distribution of chlorine are generally used to determine the
water intrusion occurs. With excessive pumping, the
source of salinity, especially when the seawater intrusion
natural hydraulic gradient towards the sea may be reversed
is the main source of groundwater contamination (Rao
and the intrusion can then extend to the pumping borehole
et al. ; Kim et al. ). When groundwater salinization
which becomes saline.
results from several processes, the isotopic analyses of δ2H,
Numerous studies deal with groundwater salinization
δ18O and 87Sr/86Sr are more efficient in identifying the poss-
(Kim et al. ; Ghabayen et al. ; Rosenthal et al.
ible origins of saline groundwater ( Jorgensen et al. ).
; Gattacceca et al. ; De Montely et al. ;
Seawater intrusion processes may be considered as a
doi: 10.2166/aqua.2013.105
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multivariate problem, which involves several parameters
via their own private wells to satisfy their water requirements.
such as hydrochemical properties, cationic exchanges and
Extremely low recharge rates of the aquifer and the ground-
transport parameters (Boluda-Botella et al. ).
water overexploitation resulted in fresh water/salt water
The objective of this study is to recognize and identify
mixing and therefore groundwater salinization.
the groundwater salinization origins of the Djeffara confined aquifer using hydrochemical and hydrodynamic analyses. Expected results shall be of paramount importance in a region characterized by an arid climate and fresh water scarcity.
Geological, structural and hydro-geological contexts The coastal Djeffara aquifer is logged in Mio-Pliocene sands. Trapped between marls and clays, the aquifer thickness varies from 25 to 80 m, with a maximum in the coastal area (Trabelsi et al. ). The depth of water-bearing hor-
STUDY AREA
izons does not exceed 300 m. The recharge of the Djeffara
The Djeffara aquifer located in Southern Tunisia (Figure 1) constitutes
the
main
water
reserve
in
this
region.
aquifer mainly comes from the ‘Continental Intercalaire (C.I)’ Aquifer through the Elhamma and Medenine faults (Figure 2). It is assured by lateral flow into upper cretaceous
Southeastern Tunisia is characterized by weak rainfall, with
and pontien layers. Recent recharge is limited and constitu-
an average annual precipitation of less than 250 mm. Rainfall
tes a small fraction of the aquifer resources (Mamou et al.
runoff is torrential causing more streaming and very low infil-
). The groundwater piezometric maps showed that
tration. Unlike temperate zones, the studied area is characterized by high temperature, and a high rate of evaporation. Intensive groundwater abstraction during the last decades has caused aquifer piezometric level decline and groundwater quality degradation. Since the year 2000, two desalinization units (Jerba, Zarzis) have been pumping together about 50,000 m3 day 1 from the Djeffara aquifer. Moreover, numerous hotels in the region pump groundwater
groundwater flows mainly in the South-West North-East direction. The study region is affected by numerous faults orientated NW–SE (Figure 2) (Floridia ; Busson ; Perthuisot ; in Jedoui ). Their extension in depth remains to be identified. These faults seem to affect the continuity and the geometry of the aquifer. Two faults concern the sea area between Jerba Island and Jorf. A communication between the aquifer and the sea through these faults is a strong possibility (Figure 3).
Figure 2 Figure 1
|
Location map of the study area (southeast Tunisia).
|
Structural map of Tunisian Djeffara showing the fault system with predominant orientation; northwest–southeast.
78
Figure 3
A. Kharroubi et al.
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Seawater intrusion in Djeffara confined aquifer
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Geological cross-section of studied area highlighting the fault systems as well as their depth extension (Mekrazi (1974), modified).
Sampling and analysis
present state. Comparing a few isolated values of the present groundwater level to the 1950 piezometric map, ground-
Field investigations were carried out from January to March
water level decline is shown to be about 27.5 m between
2010. In total, 24 groundwater samples were taken from
1950 and 2010. In areas where the water table is declining,
wells located all over the study area. A particular interest
the hydraulic head drops may promote seawater intrusion.
was attached to areas suspected to suffer seawater intrusion.
Fresh water salinization is explained by mixing between
Groundwater temperature and electrical conductivity (EC)
groundwater and seawater: (a) at the aquifer outlet, assumed
were measured in the laboratory using a thermometer and
to be northeast of Jerba Island, (b) through the numerous
conductivity electrodes, respectively. Water salinity was cal-
faults located in the marine area between Jerba Island and
culated using EC. Major elements and Br concentrations
the continent.
were analyzed using ionic liquid chromatography. Groundwater level fluctuation was continually measured by an automatic piezometer installed in the well.
Seawater intrusion mechanism Analytical solutions to approximate the seawater intrusion
RESULTS AND DISCUSSION
behavior have been derived since 1901. Under hydrostatic conditions, assuming an homogenous aquifer and steady-
Decline of the aquifer piezometric level
state freshwater flow, the depth of freshwater/saltwater interface can be shown by a model called the Ghyben–
Groundwater piezometric data of the Djeffara aquifer have
Herzberg relation. Assuming that seawater intrusion
been measured with respect to mean sea level since 1950.
comes mainly through faults and taking into account the
Data used to establish piezometric maps were provided by
groundwater level, the depth of the aquifer, fresh water den-
the ‘Regional Agricultural Department of Medenine’.
sity and seawater density (Figure 5), the groundwater
Groundwater piezometric level maps for the years 1950
piezometric level at which a new equilibrium of the sharp
and 1970 (Figures 4(a) and 4(b), respectively) and the pre-
interface is re-established can be determined. The equili-
sent groundwater level observed in several wells allowed
brium piezometric level (H*) can be expressed, using the
us to establish the groundwater level decline of the aquifer.
Ghyben–Herzberg relation, by the following equation:
In fact, because of permanent pumping in Jerba Island, mainly to supply water drinking demands, it is near impossible to establish a groundwater level map describing its
H ¼
ρ1 1 H1 ρ2
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Figure 5
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Seawater intrusion mechanism scheme showing the communication process between the aquifer and the lagoon.
the water table to the interface is balanced by a saltwater column extending from the sea level to the same depth. The transition zone between sea water and the aquifer fresh water is not a distinct boundary but a transition zone characterized by a mixing of fresh and saline waters. The Ghyben–Herzberg model is used to understand the salinization process of the Djeffara confined aquifer. It can be deduced that when the piezometric level (H ) in the aquifer is greater than H*, the flow is from the aquifer to the sea. Otherwise, the flow is from the sea to the aquifer and seawater intrusion occurs. In the case of the Djeffara aquifer, H1 ¼ 300 m, ρ1 ¼ 1,032 kg m 3, and ρ2 ¼ 1,003.5 kg m 3. Thus, H* ¼ 9.44 m. It can be concluded, therefore, that seawater intrusion occurs through the faults system when the piezometric level is less than 9.44 m. The actual groundwater level in the study area is less than 8 m. The weight of the fresh water cannot balance the weight of saltwater and the flow is from the sea to the aquifer. Figure 4
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(a) Groundwater piezometric map for the year 1950 established using piezometric data collected in wells of the study area. (b) Groundwater piezometric map for the year1970 established using piezometric data collected in wells of the study area.
Communication between the aquifer and the sea evidence
where H1 is the distance between sea level and the aquifer
The seawater intrusion in the aquifer can be confirmed
(m), ρ1 is the seawater density (kg m 3) and ρ2 is the fresh
based on the groundwater level fluctuation observed in
water density (kg m 3).
some wells near the faults (Figure 6). Two wells, located at
The Ghyben–Herzberg relation is an analytical model
approximately 800 m from the faults, showed that ground-
which describes the mixing between fresh water and sea
water level fluctuations are closely linked to sea level
water. It assumes that under hydrostatic conditions, the
variations. Simultaneous measurements of the sea wave
pressure of a unit freshwater column extending from
and the groundwater level in well No. G12, show that
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because of the excessive extraction rates from the Djeffara aquifer. Origin of salinization Geochemical analysis is considered to investigate the origin of groundwater salinization. Chlorine can be used to distinguish between several mixing mechanisms of fresh Figure 6
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Piezometric level fluctuation in a well near the sea. Fluctuation in the groundwater level decreases going to the backwaters.
water and saline water (Kim et al. ). The concentration of some minor elements such as Br is considered to be a good marker of seawater intrusion. It can be used to separ-
these two phenomena are perfectly correlated (Figure 7).
ate salinity of marine and non-marine origins (Andreasen &
The fluctuation of the groundwater level which is only
Flek ). The Br/Cl ratio remains constant when saliniza-
observed for the nearest two wells, disappears away from
tion of fresh water is related to seawater and groundwater
the fault system. This behavior can be explained by the
mixing. When the Br/Cl ratio exceeds the normal seawater
fact that the amplitude of the fluctuation is gradually
range (0.0036), potential sources of Br other than seawater
damped with increased distance from the source of the
may be responsible for water salinity. Groundwater samples
signal. Thus, it seems that the assumption of seawater intru-
from selected wells were collected and analyzed to deter-
sion in the Djeffara confined aquifer through faults is quite
mine principally Br and Cl content. The analysis (Table 1)
credible and warrants more detailed investigations to be
showed that most of the treated samples present a significant
definitively demonstrated.
Br concentration.
The fluctuation of the groundwater level depending on
The principal origin of Br in hydrogeological systems is
the tide cannot be the result of a pumping effect. Indeed,
seawater because rock bromide concentrations do not
the additional stress due to the increase of the water level
exceed 6 ppm. High Br concentration in the groundwater
in the lagoon is too small to justify such a fluctuation of
indicates the evidence of mixing between fresh and saline
the piezometric level in the aquifer.
waters. The Br/Cl diagram (Figure 9) was established to determine the origin of groundwater salinity. As Br is a good marker of seawater intrusion, high Br concentration
Salinity
in the Djeffara aquifer coupled with the abnormal salinity values indicate a seawater intrusion to a large extent. A
The groundwater salinity map established using EC values
Br/Cl ratio close to 0.0036 characterizes a fresh aquifer
(Figure 8), shows the distribution of water salinity of the
water contamination. Figure 8 shows that the majority of
aquifer. High values are observed in the northern and
points are near the mixing line, implying thereby that Cl
the eastern sides of the study area. Groundwater near the
and Br have the same origin. Areas affected by marine intru-
coast is associated with the highest salinity, with a maximum
sion are distinguished by Br/Cl ratios similar to those of
1
of 7 g l . Abnormally high salinity values are observed in
seawater. Therefore, bromide analyses showed that ground-
areas of low hydraulic heads and near the presumed aquifer
water salinity is mainly explained by freshwater/seawater
1
outlet. Relatively fresh waters (2.2 g l ) are found mainly in
mixing. Groundwater containing a significant amount of
the southern part near the recharge zone. Water salinity
Br is located beyond the fault system (Figure 10). This find-
remains almost constant within a radius of about 70 km
ing highlights the major role of faults in the transport
from the recharge zone. Beyond this distance, a sudden
process of salt waters from the sea to the aquifer.
increase in salinity is found predominantly in the northern
SO2 4 /Cl ratio has been recognized to be a good natu-
part of Jerba Island and Zarzis Region. High salt content
ral indicator of seawater intrusion in coastal aquifers
in the groundwater is probably due to seawater intrusion
(Pulido-leboeuf et al. ; Kouzana et al. ; Zouhri
81
Figure 7
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Seawater intrusion in Djeffara conďŹ ned aquifer
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Piezometric level and sea level measured simultaneously to show the correlation between the tide and the piezometric level of the aquifer.
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Figure 9
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Bromide versus chlorine concentrations established for the aquifer waters collected from wells located in the study area.
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Figure 8
Groundwater salinity map showing a marked increase in salinity values ranging from the recharge area to the suspected outlet.
Table 1
Sample
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Br, Cl, SO4, Na and Ca concentrations in the Djeffara aquifer Chloride
Bromide
Sulfate
Sodium
Calcium
(ppm)
(ppm)
(ppm)
(ppm)
(ppm)
GB1
612
0
1,723
528
182
MR1
629
0
1,570
542
187
KT1
590
0
1,640
512
168
JF1
1,696
4.98
2,550
1,240
212
BG1
1,502
5.21
2,589
980
227
G1
1,794
5.23
2,406
1,318
281
G2
1,437
5.09
1,906
1,347
265
G4
1,964
6.82
2,248
1,546
369
G6
1,769
5.36
1,872
1,358
208
G7
2,195
7.44
2,191
1,583
117
G8
2,282
6.1
2,234
1,600
281
G9
2,492
0
2,151
1,700
300
G10
1,690
5.03
2,406
1,107
369
G11
1,641
5.1
2,191
1,108
393
G12
1,618
5.02
2,204
1,093
371
BR1
2,405
7.75
2,366
1,900
381
TM1
3,201
9.96
2,061
2,059
361
ZR2
2,235
6.15
2,247
1,420
320
ZR3
2,279
7.58
2,442
1,470
288
ZR4
2,082
5.77
2,579
1,360
264
ZR5
2,158
6
2,701
1,415
248
ZR6
2,333
6.51
2,481
1,524
269
ZR7
2,423
8
2,865
1,620
296
ZR8
2,352
6.16
2,236
1,560
212
Figure 10
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Figure 11
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Localization of seawater intrusion area in the Djeffara confined aquifer.
SO4/Cl ratio versus Cl concentration in aquifer water. This highlights the contributions of the rock and sea water to underground water mineralization process.
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intrusion was confirmed by the obtained Br/Cl and SO4/Cl ratios, which are close to those of seawater. Areas of the aquifer downstream of the fault system were shown to be highly contaminated, thereby preventing any groundwater use. Therefore, seawater intrusion and groundwater quality shall be monitored to establish integrated water management strategies and preserve the limited water resources of the region.
REFERENCES Figure 12
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Chemical facies of underground waters sampled in the Djeffara deep aquifer.
et al. ). This ratio decreases when the proportion of sea water in the aquifer increases. Low SO2 ratios 4 /Cl
(Figure 11) indicate evidence of saltwater/freshwater mixing in some parts of the aquifer. However, a plot of þ 2þ Cl /SO2 leads to identification 4 as a function of Na /Ca
of Na-SO4 and Na-Cl chemical facies of underground water (Figure 12). The sodium chloride pole demonstrates the evidence of seawater/freshwater mixing. Although the current contamination level seems to be not very significant, the high pumping rates in the aquifer may magnify the seawater intrusion phenomenon in the coming years.
CONCLUSION The Djeffara aquifer abnormal salinization is mainly related to seawater intrusion and freshwater/seawater mixing. High pumping rates disturb the natural equilibrium between fresh and saline waters, resulting in the subsidence of the groundwater table below sea level, which causes seawater intrusion into the aquifer. Although seawater intrusion at the aquifer outlet is not excluded, the fault system is believed to be predominant in the process of groundwater salinization. Seawater intrusion in the aquifer through the fault system was confirmed based on the groundwater level fluctuation observed in wells near the faults. Hydrochemical analyses, based on Cl and Br ions, showed that changes of groundwater quality and high degrees of groundwater salinization are especially controlled by the mixing process. Seawater
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First received 20 September 2012; accepted in revised form 8 August 2013. Available online 7 October 2013