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Results of Kern Method

Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

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Page 1: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Results of Kern Method

Page 2: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Basic Kinematic Details

Group No.

Tube Side

Velocity (m/s)

Number of Tubes

Shell Diameter

length STHX

(m)

Ds/L

1

2

3

4

5

Page 3: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Performance Details

Group No.

Number of Tubes

Tube side Re

Shell side Re

Tube side h

(W/m2.K)

Shell side h

(W/m2.K)

1

2

3

4

5

Page 4: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Performance Details

Group No.

Tube side p, Pa

Shell side p, kPa

Uclean Ufouled

1

2

3

4

5

Page 5: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Actual Shell Side Heat Transfer Coefficient :Bell-Delaware Method

P M V SubbaraoProfessor

Mechanical Engineering Department

I I T Delhi

Five corrections to Cross Flow Heat Transfer…..

Page 6: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5
Page 7: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Shell-side heat transfer coefficient

Where hi is heat transfer coefficient for ideal cross flow past a tube bank.

Jc : Segmental baffle window correction factor Jl : Correction factors for baffle leakage effects for heat transferJb : Correction factors for bundle bypass effects for heat transfer Js : Heat transfer correction for unequal baffle spacing at inlet and/or outlet.Jr : correction factor for adverse temperature gradient in laminar flow

rsblcis JJJJJhh

Page 8: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Heat transfer coefficient for Ideal Cross Flow

14.0

,

32

ws

s

sps

s

m

spsii C

k

S

mCjh

Page 9: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Area for Ideal Cross Flow

Page 10: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Selection of Shell Diameter

A simple but reasonably accurate correlation was developed by Bell’s Group for single pass.

2

278.0

T

ctltubes PCL

DN

CL is tube layout constant , CL =0.87 for 30º and 60º layouts or CL=1.0 for 45º and 90º layouts.

For multipass arrangement, a correction factor ψn must be used to account for the decrease of tube count due to tube pass

Page 11: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5
Page 12: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

2Re33.1

1a

s

a

o

Ti

dP

aj

Where 43

Re14.01 as

aa

2Re33.1

1b

s

b

o

Ti

dP

bf

Where 43

Re14.01 bs

bb

s

outertube

s

ss

d

A

m

Re

Shell-Side Reynolds Number

14.0

,

32

ws

s

sps

s

m

spsii C

k

S

mCjh

Page 13: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Coefficients of Correlations

Page 14: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5
Page 15: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Baffle Geometry

Page 16: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Segmental baffle window correction factor, Jc

cc FJ 72.055.0

2

sin

3602121 ctlctl

twC FF

Page 17: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Segmental Baffle Cut Geometry

Segmental baffle cut height :Lbch

Page 18: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Recommended segmental baffle cut values

Page 19: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Jl : Correction factors for baffle leakage effects for heat transfer

Ssb is the shell-to-baffle leakage area.

Stb is the tube-to-baffle hole leakage area.

Sm is the cross flow area at the bundle centerline

Page 20: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Shell-to-baffle leakage area

• The shell-to-baffle leakage area within the circle segment occupied by the baffle is calculated as:

Lsb is the diametral leakage clearance between the shell diameter and the baffle diameter, Db .

Page 21: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Tube-to-baffle hole leakage area for one baffle

The total tube-to-baffle leakage area within one baffle is Stb.

Page 22: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Correction factors for bundle bypass effects for heat transfer Jb, and pressure drop Rb

ptlotlsb LDDBS m

bsbp S

SF

Lptl =0 for single pass

Page 23: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5
Page 24: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Unequal Baffle Spacing

Page 25: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Heat transfer correction for unequal baffle spacing at inlet and/or outlet, Js

n is approximately a constant, found to be 0.6 for laminar flow and 0.333 for turbulent flow.

If L* is larger than 2, it would be considered poor design, especially if combined with low Nb .

In such cases an annular distributor or other measures should be used.

Page 26: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Heat transfer correction factor for adverse temperature gradient in laminar flow

where Nc is the total number of tube rows crossed in the entire heat exchanger:

Page 27: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5
Page 28: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5
Page 29: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5
Page 30: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5
Page 31: Results of Kern Method Basic Kinematic Details Group No. Tube Side Velocity (m/s) Number of Tubes Shell Diameter length STHX (m) Ds/L 1 2 3 4 5

Shell side Fluid Flow in STHE