CHEMICAL ENGINEERING

(Amelia) #1

292 CHEMICAL ENGINEERING VOLUME 1 SOLUTIONS


If the velocity within the boundary layer may be represented by a sine function:



ux/us Dsin[
/ 2
y/υ ] ii

the integral:


∫l

0

ux
usux dyDu^2 sυ

∫ 1


0


ux/us
1 
ux/us d
y/υ

and, substituting from equation (ii):


∫l

0

ux
usux dyDu^2 sυ

∫ 1


0

[sin
/ 2
y/υ sin^2
/ 2
y/υ ]d
y/υ

Du^2 sυ

{


[


 
2 / cos[
/ 2
y/υ ]

] 1


0 ^0.^5


∫ 1


0


1 cosy/υ d
y/υ

}


Du^2 sυf 
2 / 0. 5 C

[


1 /sin
y/υ

] 1


0 g
Du^2 sυ
2 / 0. 5 D 0. 1366 u^2 sυ

From equation (ii): uxDussin[
/ 2
y/υ ]


∴ dux/dyDus
/ 2 υ cos[
/ 2
y/υ ]


and whenyD0:


dux/dyyD 0 D
/ 2
us/υ

But: R 0 D dux/dy yD 0 D
/ 2
us/υ


Therefore, substituting in equation (i):


∂/∂x
0. 1366 u^2 sυ D
/ 2
us/υ
υdυD
/us
/ 0. 2732 dx
υ^2 /xD
x/us
/ 0. 2732
υ^2 /x^2 D
/usx
/ 0. 1366

and:
υ/x D 4. 80 Rex^0.^5


PROBLEM 11.10


Derive the momentum equation for the flow of a viscous fluid over a small plane surface.
Show that the velocity profile in the neighbourhood of the surface can be expressed
as a sine function which satisfies the boundary conditions at the surface and at the outer
edge of the boundary layer.
Obtain the boundary layer thickness and its displacement thickness as a function of the
distance from the leading edge of the surface, when the velocity profile is expressed as a
sine function.

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