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ejercicios calor e intercambiadores, Monografías, Ensayos de Calor y Transferencia de Masa

ejercicios resueltos sobre transferencia de calor y intercambiarores de calor

Tipo: Monografías, Ensayos

2020/2021

Subido el 27/02/2022

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Module 7: Solved Problems
1. Deionized water flows through the inner tube of 30-mm diameter in a
thin-walled concentric tube heat exchanger of 0.19-m length. Hot
process water at 95C flows in the annulus formed with the outer tube
of 60-mm diameter. The deionized water is to be heated from 40 to
60C at a flow rate of 5 kg/s. The thermo physical properties of the
fluids are:
DEIONIZED
WATER PROCESS
WATER
kg/m3) 982.3
4181
0.643
548
3.56
967.1
4197
0.673
324
2.02
cp(J/kg.K
k(W/m.K
N.s/m2
pr
(a) Considering a parallel-flow configuration of the heat exchanger,
determine the minimum flow rate required for the hot process
water.
(b) Determine the overall heat transfer coefficient required for the
conditions of part a.
(c) Considering a counter flow configuration, determine the minimum
flow rate required for the hot process water. What is the
effectiveness of the exchanger for this situation?
pf3
pf4
pf5
pf8
pf9
pfa
pfd

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Module 7: Solved Problems

1. Deionized water flows through the inner tube of 30-mm diameter in a

thin-walled concentric tube heat exchanger of 0.19-m length. Hot

process water at 95C flows in the annulus formed with the outer tube

of 60-mm diameter. The deionized water is to be heated from 40 to

60 C at a flow rate of 5 kg/s. The thermo physical properties of the

fluids are:

DEIONIZED

WATER

PROCESS

WATER

kg/m3)

cp(J/kg.K

k(W/m.K

N.s/m

2

pr

(a) Considering a parallel-flow configuration of the heat exchanger,

determine the minimum flow rate required for the hot process

water.

(b) Determine the overall heat transfer coefficient required for the

conditions of part a.

(c) Considering a counter flow configuration, determine the minimum

flow rate required for the hot process water. What is the

effectiveness of the exchanger for this situation?

Schematic:

Process

water,h

Deionized

water,c

T c,i =40 C

T h,i =95 C

ΔT 1 T^2

mc=5kg/s

T c,0i =60 C

T h,o

T

x

Concentric tube

PF,L=0.19m

D=30mm

Assumptions: (1) Negligible heat loss to surroundings, (2) Negligible

kinetic and potential energy changes.

Analysis: (a) from overall energy balances,

.

, ,

. qmc h ThiThomc hTcoTc i

For a fixed term , ) h will be a minimum when T h,o is a minimum.

With the parallel flow configuration, this requires that Th,o=Tc,o =60C.

Hence,

Th (^) , i

. ( m

kg s J kgK C

kg s J kgK C

c T T

mc T T mh h hi ho

c co ci

  1. 85 / 4197 /. ( 95 60 )

,min , ,

.

. , ,   

(b)From the rate equation and the log mean temperature relation,

T

T

ln

T - T

2

1

1 2 , ,

 

qUATlm PFTlmPF

2. Water with a flow rate of 0.05kg/s enters an automobile radiator at

400K and leaves at 330 K. The water is cooled by air in cross flow

which enters at 0.75kg/s and leaves at 300K. If the overall heat

transfer coefficient is 200W/m

2

.K, what is the required heat transfer

surface area?

Schematic:

Water T (^) h,i =400K

m (^) h=0.05kg/s

Tc,i =300K

m (^) c=0.75kg/s

Air

Th,o=330K

Tc,o

Assumptions: (1) Negligible heat loss to surroundings and kinetic and

potential energy changes, (2) Constant properties.

Analysis: The required heat transfer rate is

q ( mc ) h ( Th , i Th , o ) 0. 05 kg / s ( 4209 J / kg. K ) 70 K 14 , 732 W

.    

Using the -NTU method,

max

min max , ,

max

min

q q W W

and

henceC C T T W K K W

C C W K

C C W K

hi ci

c

h

From figure, NTU1.5, hence

2 2 ANTU ( C min / U ) 1. 5  210. 45 W / K ( 200 W / m. K ) 1. 58 m

Comments: (1) the air outlet temperature is

T (^) c , oTc , iq / Cc  300 K ( 14 , 732 W / 755. 25 W / K ) 319. 5 K

(2) Using the LMTD approach, ΔTlm=51.2 K, R=0.279 and P=0.7.

Hence from fig F0.95 and

/ ( 14 , 732 )/[ 0. 95 ( 200 /. ) 51. 2 ] 1. 51.

2 2 Aq FUTlmW W m K Km

NTU -ln(1- ) ln( 1 0. 62 ) 0. 97

since C /C 0,

, /( [ ]) 3. 46 10 / 86 , 400 / ( 65 ) 0. 62

min max

6 min , ,

6 min , ,

hence  q C T T W W K K

C C q T T W K W K

hi ci

c co ci

And

m C c W K J kgK kg s

A NTUC U W K W m K m

c (^) c / pc 86 , 400 / / 4178 /. 20. 7 /

,

.

min

(b) using the final overall heat transfer coefficient, find

Since C min /Cmax0,

m q h W J kg kg s

T T W K K W

NTU

h fg

hi ci

hence, q C ( ) 0. 384 ( 886 , 400 / ) 65 2. 16106

1 exp( ) 1 exp( 0. 485 ) 0. 384

6 6

.

min , ,

Comments: The significant reduction (38%) in represents a

significant loss in turbine power. Periodic cleaning of condenser

surfaces should be employed to minimize the adverse effects of

fouling.

m h

.

4. Water at 225 kg/h is to be heated from 35 to 95C by means of a

concentric tube heat exchanger. Oil at 225kg/h and 210C, with a

specific heat of 2095 J/kg.K, is to be used as the hot fluid. If the

overall heat transfer coefficient based on the outer diameter of the

inner tube if 550W/m

2

.K, determine the length of the exchanger if the

outer diameter is 100mm.

Schematic:

Assumptions: (1) Negligible heat loss to surroundings, (2) Negligible

kinetic and potential energy changes, (3) Constant properties.

Properties: Table for Water:

( T (^) c ( 35 95 ) C / 2 338 K ): cp , c 4188 J / kg. K

_    

Analysis: From rate equation with Ao=DoL, L=q/U oDoΔT m

The heat rate, q, can be evaluated from an energy balance on the cold

fluid,

J kgK K W s h

kg h q mc cc Tc Tci 4188 /. ( 95 35 ) 15 , 705 3600 /

.      

In order to evaluate ΔT m, we need to know whether the exchanger is

operating in CF or PF. From an energy balance on the hot fluid, find

C

kgK

J

s h

kg h T (^) h oThiq mhchCW   

  1. 1 .

.

, ,

5. Consider a very long, concentric tube heat exchanger having hot and

cold water inlet temperatures of 85 and 15C. The flow rate of the hot

water is twice that of the cold water. Assuming equivalent hot and

cold water specifies heats; determine the hot water outlet temperature

for the following modes of operation (a) Counter flow, (b) Parallel

flow.

Schematic:

Th,i=85 C

Tc,i =15 C

Cc

Ch=2Cc

Assumptions: (1) equivalent hot and cold water specific heats, (2)

Negligible Kinetic and potential energy changes, (3) No eat loss to

surroundings.

Analysis: the heat rate for a concentric tube

Heat exchanger with very large surface area

Operating in the counter flow mode is

qq max  C min( Th , iTc , i )

Combining the above relation and rearranging, find

hi ci h i h

c hi ci hi h

h o T T T C

C

T T T

C

C

T , , , , , ,

min ,  (^  )  (  )

Substituting numerical values

T (^) h o   ( 85  15 ) C  85  C  50  C 2

,

For parallel flow operation, the hot and cold outlet temperatures will

be equal; that is T c,o=Th,o. Hence

C (^) c ( Tc , oTc , i ) Ch ( Th , iTh , o )

Setting Tc,o=Th,o and rearranging

T C C

C

C

T

C

C

T T

ho

h

c ci h

c ho hi

  

,

, , ,

Comments: Note that while  =1 for CF operation, for PF operation

find = q/q max=0.67.

q mhcphThi Tci kg s J kgK C W

5

. ,

.  , (  ) 0. 5 / ( 2650 /. )( 100  60 )  0. 53  10

5 5

 q q max    

(b)

C

kg s J kgK

C

m c

q T T

c pc

c o ci   

5

.

,

, ,

Since T c,o<Th,o, a parallel flow mode of operation is possible.

However, with (Cmin/Cmax ) = ( / , )=0.63,

.

,

. m (^) hcp (^) h mccp c

From fig (NTU) PF0.95, (NTU) CF0.

Hence

(ACF/APF)= (NTU) CF/ (NTU) PF (0.75/0.95)=0.

Because of the reduced size requirement, hence capital investment,

the counter flow mode of operation is preferred.