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/υsin^2
/ 2
y/υ]d
y/υ
Du^2 sυ
{
[
2 /cos[
/ 2
y/υ]
] 1
0 ^0.^5
∫ 1
0
1 cosy/υd
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 υcos[
/ 2
y/υ]
and whenyD0:
dux/dyyD 0 D
/ 2
us/υ
But: R 0 D dux/dyyD 0 D
/ 2
us/υ
Therefore, substituting in equation (i):
∂/∂x
0. 1366 u^2 sυD
/ 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/xD 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.