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The solutions to problem 1 and problem 2 from homework 2 of the sp. Topics: fluid dynamics course (math 292) in spring 2010. The problems involve applying reynolds transport theorem and deriving the eulerian form of the momentum equation. Problem 3 is an example of the difference between streamlines, streaklines, and pathlines in a two-dimensional flow field.
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Due before class on 03 February 2010. List any resources used in your solution and the names of students you work with.
Problem 1: (a) Consider a volume V (t) with surface S(t) with outward normal n(x, t) at time t, and S moves with the velocity field u(x, t). In class, we showed that for any vector or scalar field φ(x, t) (Reynolds Transport Theorem),
D Dt
V (t)
φdV =
V (t)
∂φ ∂t
dV +
S(t)
φ u · n dS. (1)
Assuming that φ(x, t) is a scalar, show that this can be written
D Dt
V (t)
φdV =
V (t)
Dφ Dt
dV.
(b) Consider the Eulerian form of the momentum equation:
∫
V (t)
∂(ρu) ∂t dV +
S(t)
(ρu)u · n dS = F, (2)
for external forcing F. Show that Eq. 2 can be written as simply ∫
V (t)
ρ Du Dt
dV = F. (3)
Starting with Eq. 2, you will want to apply the Divergence theorem for dyads.
Problem 2: If V (t) is a material volume and x is the position vector relative to a fixed origin, show that D Dt
V (t)
ρ(x × u) dV =
V (t)
ρ(x × Du Dt
) dV.
This result shows that the rate of change of angular momentum of the fluid is equal to its moment of fluid acceleration.
Problem 3: As an example of the difference between streamlines, streaklines, and pathlines, con- sider the two-dimensional flow field u(x, t) = (u(x, t), v(x, t), 0), where
u = x(1 + 2 t), v = y.
Compare the streamline through the point (1,1) at time t = 0 with the pathline for a particle released at (1,1) at time t = 0, and also with the streakline at t = 0 produced by tracers released from (1,1). Show your results in a comparative graphical plot.