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Homework assignment on Navier-Stokes Equations
Typology: Exercises
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16.100 Homework Assignment # 6
Due: Monday, October 31 9am
Reading Assignment
Anderson, 3
rd edition: Chapter 15, Sections 1-4, 7
Chapter 16, pages 745-751, 781-
Problem 1
y
Consider an initially stationary, long flat plate. At time t = 0 , the plate is set in motion at
velocity U. As time evolves, the air above the plate will begin to move as the viscous effects
diffuse the momentum away from the plate. We will define the height of the boundary layer of
non-negligible momentum,
0
δ ( t ), as the y-location at which the velocity is only 1% of the wall
velocity. Assume the flow is incompressible.
a) Apply the conservation of mass in differential form (i.e. not integral form) to show that
the vertical velocity, v , is zero everywhere in the flow for all time.
b) Next, show that the conservation of x-momentum can be reduced to the following form:
2
2
y
u
t
u
∂
c) Show that the following x-velocity is a solution to Equation (1) and that it satisfies the
initial and boundary conditions:
( )
( ) ∫
− ≡
≡
= −
η ξ ξ π
η
η ν
η
0
0
2 2
4
1
erf e d
y t
erf U
u
Note that erf ( )η is known as the error function and its values are available in Matlab and
Excel using the erf function.
as a function of time. For air at standard day conditions, at what time does the boundary
layer thickness reach 1 inch above the plate? What time for 1 foot above the plate?
e) Determine the skin friction coefficient c (^) f as a function of time where
f
wall
U wall
y
=
ρ
1
2 0
2
0
c (^) f 0
2
Plot as a function of U t. As time proceeds, is the plate easier or harder to keep
moving at the same velocity? Notice that at t = 0 , the skin friction has some rather large
values. Obviously, in a real situation, the friction does not reach these values. What basic part in the specification of the problem is the cause for this? Hint: it is not the
infinite length of the plate.
Problem 2
Consider the flow between two concentric cylinders as shown below:
parallel such that the radial velocity, ur , is equal to zero.
a) Using the continuity equation, show that the circumferential velocity, u (^) θ, is independent of
b) Using the circumferential momentum equation, and applying boundary conditions, determine
the circumferential velocity.
c) Without solving directly for the static pressure, use the radial momentum equation to show
that the static pressure must increase with increasing radius.