Fluid Dynamics Homework 2: Reynolds Transport Theorem and Momentum Equation - Prof. Michae, Assignments of Mathematics

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.

Typology: Assignments

Pre 2010

Uploaded on 03/28/2010

koofers-user-qhg
koofers-user-qhg 🇺🇸

9 documents

1 / 1

Toggle sidebar

This page cannot be seen from the preview

Don't miss anything!

bg1
MATH 292: Sp. Topics Fluid Dynamics - HW 2 Spring 2010
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 Smoves
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 ZV(t)
φdV =ZV(t)
∂φ
∂t dV +ZS(t)
φu·ndS. (1)
Assuming that φ(x, t)is a scalar, show that this can be written
D
Dt ZV(t)
φdV =ZV(t)
Dt +φ · udV.
(b) Consider the Eulerian form of the momentum equation:
ZV(t)
(ρu)
∂t dV +ZS(t)
(ρu)u·ndS =F,(2)
for external forcing F. Show that Eq. 2 can be written as simply
ZV(t)
ρDu
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 xis the position vector relative to a fixed origin, show
that D
Dt ZV(t)
ρ(x×u)dV =ZV(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.
1

Partial preview of the text

Download Fluid Dynamics Homework 2: Reynolds Transport Theorem and Momentum Equation - Prof. Michae and more Assignments Mathematics in PDF only on Docsity!

MATH 292: Sp. Topics – Fluid Dynamics - HW 2 Spring 2010

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

  • φ∇ · u

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.