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2 Heat Exchangers Plate Style

LMTD Lecture

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LMTD Graphs and solutions with lecture

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Page 1: LMTD Lecture

2

Heat Exchangers

Plate Style

Page 2: LMTD Lecture

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Solar Water Heating

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Okotoks Solar Seasonal Storage and District Loop Simplified Schematic

Two StorySingle Family

Homes

Underground ThermalStorage Located Beneath

MRDistrict Heating

Loop (Below Grade) Connects to Homes in Community

Detached Garages withSolar Collector roofsGlycol / Water

Heat Exchanger

District Heating LoopCentral Plant OutlineLocated on MR

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Okotoks – Energy Delivery

Bore Hole Storage

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10 20 30 40 50 60

-80

-70

-60

-50

-40

-30

-20

-10

0

5

10

15

20

25

30

35

40

45

50

55

60

Energy Balancethe rate of heat transfer between the two fluid streams in the heat exchanger, Q, is,

where is the heat capacity rate of one of the fluid streams.

c

ci

m

T

&

Q0Q =0Q =

Q

s

so

m

T

&

c

co

m

T

& s

si

m

T

&

( ) ( ) ( ) ( )p s so si p c ci coQ mc T T mc T T= − = −& &

pmc&

Page 6: LMTD Lecture

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Simple Configurations

Q = qx A

and

Q = UA (∆T)

U = (1/h1 + Rwall +1/h2)-1

Heat transfer through a wall

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Simple Configurationsfor Tube & Shell

Q = UA (∆T)Need to determine ∆T.This is not straightforward as for the parallel flow case.

UA –Value & LMTDThe unit’s overall conductance or UA value is defined as the product of the overall heat transfer coefficient and the heat transfer area. For counter-flow applications, the heat transfer rate is defined as the product of overall conductance and the log-mean temperature difference, LMTD, i.e., Q UA LMTD= ⋅where the log-mean temperature difference is equal to,

ln

out in

out

in

T TLMTDTT

∆ − ∆=

⎛ ⎞∆⎜ ⎟∆⎝ ⎠

Page 8: LMTD Lecture

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Parallel Flow

Q UA LMTD= ⋅

ln

out in

out

in

T TLMTDTT

∆ − ∆=

⎛ ⎞∆⎜ ⎟∆⎝ ⎠

Counter Flow

Q UA LMTD= ⋅

ln

out in

out

in

T TLMTDTT

∆ − ∆=

⎛ ⎞∆⎜ ⎟∆⎝ ⎠

Page 9: LMTD Lecture

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From “Heat Transfer”,By Y. Cengel

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EffectivenessThe heat exchanger effectiveness, ε, is defined as the ratio of the rate of heat transfer in the exchanger, Q, to the maximum theoretical rate of heat transfer, , i.e.,maxQ

max

QQ

ε =

The maximum theoretical rate of heat transfer is limited by the fluid stream with the smallest heat capacity rate, i.e.

min

( ) ( )( ) ( )

p s so si

p ci si

mc T Tmc T T

ε−

=−

&

&

where the is the smaller of or .min( )pmc& ( )p smc& ( )p cmc&

c

ci

m

T

&

Q0Q =0Q =

Q

s

so

m

T

&

c

co

m

T

& s

si

m

T

&

NTUThe number of transfer units (NTU) is an indicator of the actual heat-transfer area or physical size of the heat exchanger. The larger the value of NTU, the closer the unit is to its thermodynamic limit. It is defined as,

min( )p

UANTUmc

=&

Page 11: LMTD Lecture

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Capacity RatioThe capacity ratio, Cr, is representative of the operational condition of a given heat exchanger and will vary depending on the geometry and flow configuration (parallel flow, counterflow, cross flow, etc.) of the exchanger. This value is defined as the minimum heat capacity rate divided by the maximum capacity rate, i.e.,

min

max

( )( )

pr

p

mcC

mc=

&

&

It is important to note that the capacity ratio will be directlyproportional to the ratio of the mass flow rates if the specificheats of the flows are fairly constant.

Effects of Capacity Ratio and NTU on Effectiveness

Page 12: LMTD Lecture

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Effectiveness Relations

Page 13: LMTD Lecture

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NTU Relations

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Refrigeration

Examples

Other TypesHeat Pipe

RotaryILC Enthalpy Wheel

Page 16: LMTD Lecture

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Heat Pipe

Enthalpy WheelThe heart of the Energy Recovery Ventilator is the desiccant coated energy recovery wheel, which slowly rotates between its two sections. In one section, the stale, conditioned air is passed through the wheel, and exhausted in the atmosphere. During this process, the wheel absorbs sensible and latent energy from the conditioned air, which is used to condition (cool / heat) the incoming Fresh Air in the other section, during the second half of its rotation cycle.