Verifying Stokes' Flow for Fluid Motion Around a Sphere

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Homework Help Overview

The problem involves analyzing the motion of a spherical object through a fluid using Stokes' equations, specifically in the context of slow velocities. The original poster seeks to verify the solution known as Stokes' Flow and to demonstrate the drag force acting on the sphere.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the appropriate coordinate system to use, with mentions of spherical coordinates and the need to express Stokes' equations accordingly. Questions arise regarding the terms in the equations and the implications of symmetry.

Discussion Status

There is an ongoing examination of the equations and terms involved, with some participants questioning the correctness of the initial setups and calculations. Guidance has been offered regarding the need to convert coordinates and clarify the components of the fluid velocity vector.

Contextual Notes

Participants note potential confusion regarding the coordinate systems used and the definitions of terms, particularly in relation to the original problem statement. There is an emphasis on ensuring that the equations are correctly expressed in spherical coordinates.

Mark Mendl
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Homework Statement


Let a spherical object move through a fluid in R3. For slow velocities, assume Stokes’ equations apply. Take the point of view that the object is stationary and the fluid streams by. The setup for the boundary value problem is as follows: given U = (U, 0, 0), U constant, find u and p such that Stokes’ equation holds in the region exterior to a sphere of radius R, u = 0 on the boundary of the sphere and u = U at infinity.
The solution to this problem (in spherical coordinates centered in the object) is called Stokes’ Flow:
stokes.png

where p0 is constant and n = r/r .
(a) Verify this solution.
(b) Show that the drag is 6πRνU and there is no lift.

If someone can help it would be great.

Homework Equations

The Attempt at a Solution


a) [/B]I started using the stokes equations but couldn't get there.
 
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Mark Mendl said:
a) I started using the stokes equations but couldn't get there.

What coordinate system did you use, and what form of the stokes equations did you use? How can we help if you don't show us what you have done so far?

Chet
 
Chestermiller said:
What coordinate system did you use, and what form of the stokes equations did you use? How can we help if you don't show us what you have done so far?

Chet
Using spherical coordinates (that is what asked in the problem I guess) and these equations
stokes2.png
 
I'm not sure about the n (U.n) term, it stays just U/r2?

Thanks,
Mark
 
Mark Mendl said:
Using spherical coordinates (that is what asked in the problem I guess) and these equations
stokes2.png
OK. Express these equations in spherical coordinates, of course without the longitudinal dependence because of symmetry.

Chet
 
Chestermiller said:
OK. Express these equations in spherical coordinates, of course without the longitudinal dependence because of symmetry.

Chet
To prove the divergence equal to zero, only the term in r exists, so we have
stokes3.png

I solved that but it's not 0, I guess the problem is in the n (U.n) term...
 
Mark Mendl said:
To prove the divergence equal to zero, only the term in r exists, so we have
stokes3.png

I solved that but it's not 0, I guess the problem is in the n (U.n) term...
This is not correct for a couple of reasons. First of all, you have written the equation for the divergence in cylindrical coordinates, rather than spherical coordinates. Secondly, you have omitted the derivative with respect to the latitudinal coordinate.

Also, please write down for me the spherical components of the fluid velocity vector in the radial direction and latitudinal direction.

Chet
 
Chestermiller said:
This is not correct for a couple of reasons. First of all, you have written the equation for the divergence in cylindrical coordinates, rather than spherical coordinates. Secondly, you have omitted the derivative with respect to the latitudinal coordinate.

Also, please write down for me the spherical components of the fluid velocity vector in the radial direction and latitudinal direction.

Chet
Yes, actually when I solved it I used the equation for spherical and not that one, I put it wrong. (it's with both r squared).
But I only used the radial direction in the fluid velocity... how do we have a latitudinal component if n and U only have terms in r?
 
.
 
Last edited:
  • #10
Mark Mendl said:
Yes, actually when I solved it I used the equation for spherical and not that one, I put it wrong. (it's with both r squared).
But I only used the radial direction in the fluid velocity... how do we have a latitudinal component if n and U only have terms in r?
The components of U they gave are for cartesian coordinates. I guess they should have mentioned that. You need to convert this to spherical coordinates.

Chet
 
  • #11
Chestermiller said:
The components of U they gave are for cartesian coordinates. I guess they should have mentioned that. You need to convert this to spherical coordinates.

Chet
So I rewrite U = (Ucosθ, Usinθ, 0), my vr will be something like -3/4*R*Ucosθ(1/r+1/r3) - 1/4R3*Ucosθ(1/r3-3/r5)+Ucosθ ?
 
  • #12
Mark Mendl said:
So I rewrite U = (Ucosθ, Usinθ, 0), my vr will be something like -3/4*R*Ucosθ(1/r+1/r3) - 1/4R3*Ucosθ(1/r3-3/r5)+Ucosθ ?
No. It looks like you have several algebra errors in there. Try again, or show more details please.

Chet
 
  • #13
Hum... how would stay n(U.n)? cos(θ)U/r? probably not...
 
  • #14
Mark Mendl said:
Hum... how would stay n(U.n)? cos(θ)U/r? probably not...
No. n is the unit vector in the radial direction. So n(U.n)=Ucosθn.

Chet
 

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