ME150_Lect17-1_LMTD Method for Heat Exchangers

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ME 150 – Heat and Mass Transfer

Chap. 17.1: LMTD Method for Heat Exchangers

Log Mean Temperature Difference for Heat Exchangers

m h = m h ,i = m h ,o

q = m h ⋅ c p ,h ⋅ (Th ,i − Th ,o )

m c = m c ,i = m c ,o

q = m c ⋅ c p ,c ⋅ (Tc ,o − Tc ,i )

Prof. Nico Hotz

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ME 150 – Heat and Mass Transfer

dq = −m h ⋅ c p ,h ⋅ dTh dq = m c ⋅ c p ,c ⋅ dTc

Chap. 17.1: LMTD Method for Heat Exchangers

⎛ 1 1 ⎞⎟ ⎜ dTh − dTc = d (Th − Tc ) = −dq ⋅ + ⎜ m ⋅ c ⎟ ⎝ h p ,h m c ⋅ c p ,c ⎠

On the other hand, the heat transfer between both sides can be calculated as: dq = U ⋅ dA ⋅ (Th − Tc )

Prof. Nico Hotz

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ME 150 – Heat and Mass Transfer

Chap. 17.1: LMTD Method for Heat Exchangers

Combining the heat transfer equation and the energy balance: ⎛ 1 1 ⎞⎟ ⎜ d (Th − Tc ) = −U ⋅ dA ⋅ (Th − Tc )⋅ + ⎜ m ⋅ c ⎟ ⎝ h p ,h m c ⋅ c p ,c ⎠ ⎛ 1 d (ΔT ) d (Th − Tc ) 1 ⎞⎟ ⎜ = = −U ⋅ + ⋅ dA ⎜ m ⋅ c ⎟  (Th − Tc ) ΔT m ⋅ c c p ,c ⎠ ⎝ h p ,h

After integration: ⎛ 1 ⎛ ΔT2 ⎞ 1 ⎞⎟ U⋅A ⎜ ⎜ ⎟ ln⎜ = − U ⋅ A ⋅ + = − ⋅ [(Th,i − Tc,i ) − (Th,o − Tc,o )] ⎟ ⎜ m ⋅ c ⎟  Δ T m ⋅ c q c p ,c ⎠ ⎝ 1 ⎠ ⎝ h p ,h q = U ⋅ A⋅

ΔTo − ΔTi ln(ΔT2 ΔT1 )

Prof. Nico Hotz

1: x = 0 2: x = L 3


ME 150 – Heat and Mass Transfer

Chap. 17.1: LMTD Method for Heat Exchangers

LMTD Method for Parallel Flow Heat Exchangers

1: x = 0, inlet for cold and hot 2: x = L, outlet for cold and hot

ΔTo − ΔTi ΔT2 − ΔT1 q = U ⋅ A⋅ = U ⋅ A⋅ ln(ΔT2 ΔT1 ) ln(ΔT2 ΔT1 )

Prof. Nico Hotz

ΔT1 = ΔTi = Th ,i − Tc ,i

ΔT2 = ΔTo = Th ,o − Tc ,o

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ME 150 – Heat and Mass Transfer

Chap. 17.1: LMTD Method for Heat Exchangers

LMTD Method for Counter Flow Heat Exchangers

1: x = 0, hot inlet and cold outlet 2: x = L, cold inlet and hot outlet

ΔT2 − ΔT1 q = U ⋅ A⋅ ln(ΔT2 ΔT1 )

ΔT1 = Th ,1 − Tc ,1 = Th ,i − Tc ,o

ΔT2 = Th , 2 − Tc , 2 = Th ,o − Tc ,i

Prof. Nico Hotz

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ME 150 – Heat and Mass Transfer

Chap. 17.1: LMTD Method for Heat Exchangers

LMTD Method for Cross Flow Heat Exchangers

P= R=

q = U ⋅ A ⋅ F ⋅ ΔTlm, cross

Tc ,o − Tc ,i Th ,i − Tc ,i Th ,i − Th ,o Tc ,o − Tc ,i

ΔTlm, cross =

(T − T )− (T ln[(T − T ) (T h ,i

h ,i

Prof. Nico Hotz

c ,o

c ,o

h ,o h ,o

− Tc ,i )

− Tc ,i )]

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ME 150 – Heat and Mass Transfer

Chap. 17.1: LMTD Method for Heat Exchangers

Overall Heat Transfer: Tcold flow Cold fluid:

Rtot = Rcold , conv + Rwall , cond + Rhot , conv

Rcold,conv Tcold wall

Wall:

Rwall,cond Thot wall

Hot fluid:

Rtot =

Rhot,conv

Thot flow

1 t 1 + + hcold ⋅ Acold k wall ⋅ Ac hhot ⋅ Ahot

U ⋅ Awet =

1 Rtot

→ qtot = U ⋅ Awet ⋅ (Thot , flow − Tcold , flow )

Prof. Nico Hotz

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ME 150 – Heat and Mass Transfer

Chap. 17.1: LMTD Method for Heat Exchangers

Log Mean Temperature Difference Method: The LMTD Method is used to design heat exchangers for known inlet and outlet temperatures of the fluids and a known geometry of the heat exchanger. Possible Procedure to Design Heat Exchanger: 1) Determine known or specified inlet and outlet temperatures. 2) Calculate total heat transfer from inlet and outlet temperatures and fluid properties. 3) Calculate LMTD using formula for the given heat exchanger configuration (parallel, counter, cross flow). 4) Calculate overall thermal resistance using q and LMTD. 5) Calculate geometry from overall thermal resistance and heat transfer coefficients.

Prof. Nico Hotz

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ME 150 – Heat and Mass Transfer

Prof. Nico Hotz

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