Arjstte 02 002

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Advanced Research Journals of Science and Technology

ADVANCED RESEARCH JOURNALS OF SCIENCE AND TECHNOLOGY

(ARJST)

Performance Analysis of Domestic Refrigerator With and Without Heat Recovering Unit by using R134a and R600a

2349-9027

Jose Philip1, S.N.CH.Dattu2, V.V Kamesh3 1 Research Scholar, Department of Thermal Engineering,Aditya Engineering College, Surampalem, Andra Pradesh, India. 2 Associate Professor,Department of Mechanical Engineering, Aditya Engineering College, Surampalem, Andra Pradesh, India. 3 Associate Professor,Department of Mechanical Engineering, Aditya Engineering College, Surampalem, Andra Pradesh, India.

Abstract This project presents a study of using different environment friendly refrigerants with zero ozone depletion potential (ODP) and minor global warming potential (GWP), to replace R134a in domestic refrigerator and waste heat recovery from condenser. This work consists of using a hydrocarbon gas mixture which does not deplete ozone layer is ecofriendly, and can be used in the commonly used refrigerators without any significant change in the system of domestic refrigerator. A house hold refrigerator designed to work with R134a was used as an investigation unit to assess the panorama of using R600a refrigerants without any modifications. The recital of the refrigerator using R600a refrigerant was investigated and a compared with the performance of refrigerator when R134a was used as refrigerant. The effect of condenser temperature and evaporator temperature on COP, refrigerating effect was investigated by using both the refrigerants. The energy consumption of the refrigerator during experiment with R600a refrigerant and R134a was measured by using energy meter. The outcome shows the permanent running and cycling results showed that R134a with a charge of 100g or R600a refrigerant with charge of 100mg or more satisfy the required freezer air temperature of -12oC. The main objective of this paper is to study “waste heat recovery system for domestic refrigerator”. An attempt has been made to utilize waste heat from condenser of refrigerator to heat water. This heat can be used for number domestic and industrial purposes. In minimum constructional, maintenance and running cost, this system is much useful for domestic purpose like heating water, heating room, etc. It is valuable alternative approach to improve overall efficiency and reuse the waste heat. The study has shown that such a system is technically feasible and economically viable and also testingtheperformancewithandwithoutheatrecovering unit.

*Corresponding Author: Jose Philip, Research Scholar, Department of Thermal Engineering, Aditya Engineering College, Surampalem, Andra Pradesh, India. Published: December 19, 2015 Review Type: peer reviewed Volume: II, Issue : II Citation: Jose Philip,Research Scholar (2015) Performance Analysis of Domestic Refrigerator With and Without Heat Recovering Unit by using R134a and R600a

INTRODUCTION Heat is energy, so energy saving is one of the key matters from view point of fuel consumption and for the protection of global environment for our future usage. So it is necessary that a significant and concrete effort should be made for conserving energy through waste heat recovery from different machineries. The main objective of this paper is to study “Waste Heat recovery system for domestic refrigerator and performance of refrigerator by using environmental friendly refrigerant”. An attempt has been made to utilize waste heat from condenser of refrigerator to heat water. A domestic refrigerator is a common household Appliance that consists of a thermally insulated compartment and which when works, transfers heat from the inside of the compartment to its external atmosphere so that the inside of the thermally insulated compartment is cooled to a temperature below the ambient temperature of the room. Heat rejection may occur directly to the air in the case of a conventional household refrigerator

having air-cooled condenser or to water in the case of a water-cooled condenser. Tetrafluoroethane (HFC134a) refrigerant was now widely used in most of the domestic refrigerators as the working fluid. THEORY OF REFRIGERATION SYSTEM It has been mentioned before that the refrigeration is defined as the process of removal of heat from a region or state or a substance to reduce and maintain its low temperature and transferring that heat to another region, state or substance at higher temperature by the help of refrigerant which one known as working fluid. The refrigeration process that employed in the domestic refrigerator is based on a vapor compression cycle as shown in Figure 2 and collaborated with Figure 1. There are three main parameter that were considered in this study; compressor power, refrigeration capacity and coefficient of performance (COP).

P-h diagram of vapor compression cycle

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Advanced Research Journals of Science and Technology

Process line from 1 to 2 represents compressor power. Compressor power is defined as the power needed to do the compression process in watt. The compressor power is determined by multiplying enthalpy change across the compressor to the mass flow rate of refrigerant, thus, P=m(h2-h1)

Normal boiling point in O C

-11.6

-26.5

Pressure at -25o C in bar

0.58

1.07

Liquid density At -25o C in kg/l

0.60

1.37

h2 = enthalpy of compressor output (KJ/Kg) h1 = enthalpy of compressor input (KJ/Kg)

Vapor density at t0 -25/+32o C in kg/m3

1.3

4.4

Meanwhile, process from point 2 to 3 represents heat rejection through condenser to atmosphere. Refrigerant get cooled and changed from vapor form to liquid the amount of heat rejected is not significant in the present study. Process from point 3 to point 4 shows throttling effect through capillary tube whereby the working pressure of refrigerant will be reduced from discharge pressure to suction pressure in low pressure region. Refrigeration capacity, which is represented by process line 4 to 1, is defined as the amount of heat absorbed by a unit mass of refrigerant in evaporator from the cooling space. The refrigeration capacity can be obtained using equation below:

Volumetric capacity at -25/55/32o C in kJ/m3

373

658

Enthalpy of vaporization at -25o C in kJ/kg

376

216

Pressure at +20o C in bar (absolute)

3.0

5.7

toxicity

LOW

MEDIUM

Flammability

~460o C - ~470O C(YES)

-800O C

Toxicity after ignition

Extremely Low

Extremely high

Lubricant flammability

~ 200o C

~200o C

Global warming potential

~ 0/3

3100/1300

Ozone depletion potential I

No

No

Atmosphere life time(Years)

<1

~16

Cooling performance @ 40O C

Excellent

Poor

Energy efficiency

High

Low

Power consumption

Low

High

Average system charge by weight

<300 grams

~840 grams

Q=m(h1-h4) h1 = enthalpy of compressor input (KJ/Kg) h2 = enthalpy of evaporator input (KJ/Kg) The coefficient of performance (COP) is a measure of efficiency of the refrigerator. The COP of a domestic refrigerator is the ratio of the refrigeration capacity to the energy supplied to the compressor. It can be expressed by equation below

Refrigerants The last decade has seen drastic changes in the selection and use of refrigerants for refrigeration and air conditioning systems, mainly in reaction to the environmental issues of ‘holes in the ozone layer’ and ‘global warming or greenhouse effect’. Previously there had not been much discussion about the choice of refrigerant, as the majority of applications could be met by the well-known refrigerants. So in this paper am discussing about the usage of R600a which is more ecofriendly than R134a which is commonly using Properties of R-134a and R600a Refrigerants with Comparison Chart Refrigerant

R 600a

R 134a

Class

HC (Hydro carbon)

HFC(Hydro Fluoro Carbon)

Name

Isobutane

1,1,1,2-Tetra Fluoro-Ethane

Formula

(CH3)3CH

CH3-CH2F

Critical temperature in O C

135

101

Boiling point @ 20O C

-29.8O C

-26.6O C

Molecular weight in kg/kmol

58.1

102

EXPERIMENTAL PROCEDURE The following procedure is adopted for experimental setup of the vapor compression refrigeration system. 1. The domestic refrigerator is selected (whirlpool ML1340, 180l), working on vapor compression refrigeration system which using R134a as refrigerant. 2. Pressure and temperature gauges are installed at each entry and exit of the compressor, exit of condenser and inlet of evaporator. 3. Flushing of the system is done by pressurized nitrogen gas. 4. R134a refrigerant is charged into the vapor compression refrigeration system as shown in the above figure. It is charging to the compressor by amount of 100g. 5.Leakage tests are done by using soap solution in every welded portion in order to further the condenser and evaporator pressure and found that there is no leakages which required the absolutely the present investigation to carry out further processing and coated with plastic tapes for safety purpose.

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Advanced Research Journals of Science and Technology

R134a-Without HRU (Heat Recovering Unit) Time

6. Power on the refrigerator and observation is required for 1 hour and take the pressure and temperature readings at each section in every one hour gap. 7. The performance of the existing system is completed, with the help of temperature and pressure gauge readings those which are connected to compressor inlet and outlet, condenser out and evaporator inlet. 8. The refrigerant is discharged out and condenser is located at the inlet of the capillary tube. 9. Temperature gauge and pressure gauge readings are took and the performance is completed by calculations and values from p-h chart. 10. After that removed R134a and charging R600a to the same system. 11. Then power on and taking values from pressure gauge and thermometer and calculating the cop, that means continuing the process same as R134a 12 After that connected water heater to the outlet of compressor and bottom of condenser tubes, this made with copper coil and again continuing the process from charging R134a (Step 4) Observations and Result Analysis T1=Compressor Inlet Temperature ( C) T2=Compressor Outlet Temperature (o C) T3=Condenser Inlet Temperature (o C) T4=Evaporator Inlet Temperature (o C) o

P1=Compressor Inlet Pressure (bar) P2=Compressor Outlet Pressure (bar) P3=Condenser Outlet (bar) P4=Evaporator Inlet (bar) h1= enthalpy (kJ/kg) according to temperature (T1) and pressure (P1) from p-h chart h2= enthalpy (kJ/kg) according to temperature (T1) and pressure (P1) from p-h chart h3= enthalpy (kJ/kg) according to temperature (T1) and pressure (P1) from p-h chart h4= enthalpy (kJ/kg) according to temperature (T1) and pressure (P1). from p-h chart Net Refrigeration Effect (NRE) = h1-h4 (kJ/kg) Amount of Compressor work= h2-h1 (kJ/kg) Heat removed through condenser= h3-h2 (kJ/kg)

T1 (oC)

T2 (o C)

T3 (oC)

T4 (oC)

P1 (bar)

P2 (bar)

P3 (bar)

P4 (bar)

10AM

20

34

28

2

1.1

12.2

11.3

0.9

11AM

29

42

32

-2

1.4

13.3

11.9

1.2

12PM

31

44

35

-4

1.6

15.3

12.7

1.4

1PM

33

47

36

-6

1.8

16.8

13.3

1.6

2PM

34

50

39

-9

2.1

17.1

14.2

1.9

Time

h1 (kJ/ kg)

h2 (kJ/ kg)

h3 (kJ/ kg)

h4 (kJ/ kg)

h1h4

h2h1

h2h3

COP

Energy Consumption (KWh)

10 AM

380

420

265

160

220

40

155

5.95

1.29

11AM

385

422

269

167

218

37

153

6.18

1.45

12 PM

389

424

272

171

218

35

152

6.22

1.57

1 PM

392

426

275

174

218

34

151

6.45

1.69

2 PM

395

430

280

175

220

35

150

6.75

1.85

R134a-With HRU Time

T1 (o C)

T2 (o C)

T3 (o C)

T4 (o C)

T WATER

P1 (bar)

P2 (bar)

P3(bar)

10AM

24

35

28

0

21

1.2

13.2

12.5

11AM

28

40

30

-2

30

1.7

18.2

16.7

12PM

33

47

32

-6

38

2.1

21.2

17.3

1PM

37

52

34

-8

42

2.4

22.2

18.2

2PM

39

55

36

-11

54

2.8

24.2

19.1

Time

h1 (kJ/ kg)

h2 (kJ/ kg)

h3 (kJ/ kg)

h4 (kJ/ kg)

h1h4

h2h1

h2h3

COP

Energy Consumption (KWh)

10AM

385

420

235

150

235

35

185

6.71

1.13

11AM

390

423

240

158

232

33

183

7.03

1.39

12PM

393

425

243

166

227

32

182

7.09

1.53

1PM

397

428

247

168

229

31

181

7.19

1.70

2PM

400

430

250

170

230

30

180

7.86

1.70

R600a-Without HRU (Heat Recovering Unit) Time

T1 (oC)

T2 (o C)

T3 (oC)

T4 (oC)

P1 (bar)

P2 (bar)

P3 (bar)

P4 (bar)

10AM

21

36

24

1

1.7

19.6

15.3

1.5

11AM

28

40

28

-3

2.3

23.3

17.4

2.1

12PM

33

47

31

-7

2.9

24.1

18.2

2.7

1PM

36

53

33

-12

3.2

24.8

18.9

3.0

2PM

39

58

36

-15

3.4

25.3

19.3

3.2

Time

h1 (kJ/ kg)

h2 (kJ/ kg)

h3 (kJ/ kg)

h4 (kJ/ kg)

h1h4

h2h1

h2h3

COP

Energy Consumption (KWh)

10 AM

580

620

280

185

395

40

340

9.87

.92

11AM

583

623

285

186

397

40

338

9.97

.99

12 PM

587

625

290

190

397

38

335

10.04

1.14

1 PM

589

626

292

192

397

37

334

10.17

1.20

2 PM

590

628

295

195

395

35

150

10.39

1.26

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Advanced Research Journals of Science and Technology

Percentage Energy Saved

R600a-With HRU Time

T1 (oC)

T2 (o C)

T3 (oC)

T4 (oC)

P1 (bar)

P2 (bar)

P3 (bar)

P4 (bar)

Time

Energy Consumption (KWh) of R134a

Energy Consumption (KWh) of R134a With HRU

% of Energy Saved

10AM

25

35

27

0

21

1.9

20.2

16.3

11AM

33

48

33

-5

30

2.6

24.6

18.9

12PM

36

54

35

-11

38

3.4

28.3

21.2

1PM

39

58

37

-14

42

3.9

29.4

24.3

10AM

1.29

1.13

14.15

28.3

11AM

1.45

1.39

4.31

12PM

1.57

1.53

2.61

1PM

1.69

1.70

-0.588

2PM

1.85

1.70

0.088

2PM

Time

40

62

38

-19

54

4.2

h2h1

h2h3

32.1

h1 (kJ/ kg)

h2 (kJ/ kg)

h3 (kJ/ kg)

h4 (kJ/ kg)

h1h4

COP

Energy Consumption (KWh)

10AM

590

625

275

225

365

36

350

10.42

1.02

11AM

594

632

278

228

366

38

354

10.63

1.02

12PM

605

634

282

230

375

29

352

12.93

1.15

1PM

609

638

288

232

377

29

350

13

1.18

2PM

615

640

290

235

380

25

350

15.2

1.24

Percentage of COP Improved TIME

COP of R134a

COP of R134a with HRU

% of COP improved

10AM

5.95

6.71

12.77

11AM

6.18

7.03

13.75

12PM

6.22

7.09

13.98

1PM

6.45

7.19

11.47

2PM

6.75

7.86

13.48

Percentage of COP improved by using HRU than normal system

Percentage of Energy Savings by using HRU in R134a System Time

Energy Consumption (KWh) of R134a

Energy Consumption (KWh) of R600a

% of Energy Saved

10AM

1.29

.92

40.21

11AM

1.45

.99

46.46

12PM

1.57

1.14

37.71

1PM

1.69

1.20

40.83

2PM

1.85

1.26

46.82

Percentage of Energy Savings by using R600a against R134a Time

Energy Consumption (KWh) of R600a

Energy Consumption (KWh) of R600a with HRU

% of Energy Saved

10AM

.92

.90

14.15

11AM

.99

1.02

-2.94

TIME

COP of R134a

COP of R600a

% of COP improved

12PM

1.14

1.15

-0.869

10AM

5.95

9.87

65.88

1PM

1.20

1.18

1.694

2PM

1.26

1.24

1.612

11AM

6.18

9.97

61.32

12PM

6.22

10.04

61.41

1PM

6.45

10.17

57.67

2PM

6.75

10.39

53.92

Percentage of Energy Savings by using HRU in R600a system Time

Energy Consumption (KWh) of R134a With HRU

Energy Consumption (KWh) of R600a with HRU

% of Energy Saved

Percentage of COP improved by using R600a against R134a TIME

COP of R600a

COP of R600a with HRU

% of COP improved

10AM

1.13

.90

25.55

10AM

9.87

10.42

5.57

11AM

1.39

1.02

36.27

11AM

9.97

10.63

6.61

12PM

1.53

1.15

33.04

12PM

10.04

12.93

28.7

1PM

1.70

1.18

44.06

1PM

10.17

13

28.7

2PM

1.70

1.24

37.09

2PM

10.39

15.2

29.1

Performance improved by using HRU in R600a system TIME

COP of R600a

COP of R600a with HRU

% of COP improved

10AM

6.71

10.42

55.29

11AM

7.03

10.63

51.20

12PM

7.09

12.93

82.36

1PM

7.19

13

80.80

2PM

7.86

15.2

83.43

Percentage of Energy Savings by using HRU with R134a & R600a

Sample Calculations For R134a (Without HRU) (For Set of Values According To 12pm) T1= 31 (o C) P1= 1.6 (bar) h1= 389 (kJ/kg) (Enthalpy values from R134a p-h Chart) T2= 44 (o C) T3= 35 (o C) T4= 4 (o C)

P2= 15.3 (bar) P3= 12.7 (bar) P4= 1.2 (bar)

h2= 424 (kJ/kg) h3= 272 (kJ/kg) h4= 171 (kJ/kg)

Percentage of COP improved by using HRU with R134a & R600a

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Advanced Research Journals of Science and Technology

Net Refrigeration Effect (NRE) = h1-h4 =218 (kJ/kg) Amount of Compressor work= h2-h1 = 35 (kJ/kg) Heat removed through condenser= h3-h2 = 152 (kJ/kg)

Comparison of COP of R134a and R600a both with HRU

Average % of COP improved (By using HRU in R134a System) = 13.07 % Average % of COP improved (By using R600a in R134a System) = 60.04% Average % of COP improved (By using HRU in R600a System) = 19.73% Average % of COP improved (By using HRU in R134a & R600a Systems) = 70.61% Average Energy consumption by R134a without HRU = 1.57 KWh Average Energy consumption by R134a with HRU = 1.49KWh

Comparison of COP of R134a and R134a with HRU

Average Energy consumption by R600a without HRU = 1.12KWh Average Energy consumption by R600a with HRU = 1.12KWh % of energy saving by using R600a in R134a System = 40.17% % of energy saving by using HRU in R600a System = 0% % of energy saving by using HRU in R134a & R600a System = 33.07 % GRAPHS

Comparison of COP of R600a and R600a with HRU

Time vs. Energy consumption in KWh Comparison of COP of R134a and R600a

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Advanced Research Journals of Science and Technology

Experimental Cases

Refrigeration Effect

COP

Energy Consumption

R134a without HRU

218

6.45

1.57KWh

R134a with HRU

230

7.20

1.49 KWh

R600a without HRU

397

10.00

1.12 KWh

R600a with HRU

375

12.50

1.12 KWh

Comparison Table TIME vs. T water Graph

Time vs. Refrigeration Effect

CONCLUSION In the present work experimental investigation is carried out to investigate the performance of vapor compression refrigeration system of a domestic refrigerator of 180 liters capacity, with R134a and R600a as refrigerants in domestic refrigerator with and without HRU. After conducting the experiments, the following conclusions are drawn. Net refrigerating effect is increased by using HRU in domestic Refrigerator by using R134a as refrigerant and light decrease in R600a refrigeration system with and without HRU. Giving more refrigeration effect than R134a by using R600a in both cases. Coefficient of performance is increased by using HRU in Domestic Refrigerator and also R600a giving more COP than R134a. R600a with HRU giving highest COP. Then R600a without HRU, R134a with HRU, least COP given by R134a without HRU. Heat to be rejected in condenser is used to heat water. While using R600a getting more hot water than R134a which shows that it is transferring more heat. Energy Consumption By using R600a is less than Energy consumption By R134a and also with and without HRU, energy Consumption By R600a is same But in R134a with HRU consuming less energy than without HRU. From the above discussions, it can be concluded that the performance of vapor compression refrigeration system of domestic refrigerator is increasing by using water heater for recovering heat. In domestic refrigerator we can directly replace R134a with R600a and the performance is increased by using R600a than R134a. Below tables shows the performance analysis results and energy consumption analysis. From table 6.2 we can conclude that by using HRU we can improve COP and energy savings in both cases of using R134a and R600a. By using R600a in R134a system, we can see that COP and Energy savings are improved. By using R600a, we are getting more performance and energy savings than R134a and it is environmental friendly also. So we can prefer R600a and also HRU also for energy savings.

Experimental Cases

% of COP improved

% of Energy Saved

Energy Consumption

By using HRU in R134a System

13.07

4.114

1.57KWh

By using R600a in R134a System

60.04

42.42

1.49 KWh

By using HRU in R600a System

19.73

2.73

1.12 KWh

By using HRU in R134a & R600a Systems

70.61

35.22

1.12 KWh

Comparison Table

References [1] S C Kaushik and M Singh, Feasibility and design studies for heat recovery from a refrigeration system with a Canopus Heat Exchanger, Heat Recovery Systems and CHP, Vol.15(1995)665673. [2]P Sathiamurthi, P S S Srinivasan, Studies on Waste Heat Recovery and Utilization. Globally Competitive eco-friendlt technologies engineering National Conference(2005)39. [3]P Sathiamurthi, P S S Srinivasan ‘‘Design and Development of Waste Heat Recovery system for air conditioning unit’’, European Journal of Scientific Research,Vol.54 No.1(2011) , pp.102-110. [4]F.N.Yu, K T Chan, ‘‘Improved Condenser design and condenser-fan operation for air-cooled chillers”,Applied Energy,Vol.83(2006)628-648. [5]H.I.Abu-Mulaweh, ‘‘Design and performance of a thermo siphon heat recovery system”,Applied Thermodynamic Engineering,Vol.26(2006)417-477. [6]P Sathiamurthi and R Sudhakaran ‘‘Effective utiluzation of waste water in air conditioner”, Energy and Environmental technologies for sustainable development-Int. Conf.Proc.(2003).

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Advanced Research Journals of Science and Technology

Author

Jose Philip, Research Scholar, Department of Thermal Engineering, Aditya Engineering College, Surampalem, Andra Pradesh, India.

V.V Kamesh Assistant Professor, Department of Mechanical Engineering, Aditya Engineering College, Surampalem, Andra Pradesh, India.

S.N.CH.Dattu Assistant Professor, Department of Mechanical Engineering, Aditya Engineering College, Surampalem, Andra Pradesh, India.

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