Question on Divergence in Cylindrical Coords

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Homework Help Overview

The discussion revolves around the divergence of a vector field in cylindrical coordinates, specifically the derivation and interpretation of the divergence operator applied to a vector field. The original poster presents a formula from their textbook and expresses confusion regarding a specific term in the divergence expression.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the derivation of the divergence in cylindrical coordinates, questioning the role of the radial and angular unit vectors and their dependence on the angular variable. Some participants suggest that the original poster's misunderstanding stems from not accounting for the vector nature of the unit vectors.

Discussion Status

The discussion is active, with participants providing insights into the relationships between unit vectors and their derivatives. There is a focus on clarifying the differences between Cartesian and cylindrical coordinates, particularly regarding how unit vectors behave in these systems. While some participants express confusion, others offer explanations that may help guide understanding.

Contextual Notes

Participants are navigating assumptions about the behavior of unit vectors in cylindrical coordinates and how these relate to the divergence operation. There is an emphasis on understanding the mathematical relationships rather than deriving a final solution.

Spectre5
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Hey, I have a question on a derivation

The following is in my textbook (V = vector):

[tex]\nabla \cdot V = \frac {1}{r} \frac {\partial{(rV_{r}})}{\partial{r}} + \frac {1}{r} \frac {\partial{V_{\theta}}}{\partial{\theta}} + \frac {\partial{V_{z}}}{\partial{z}}[/tex]

where:

[tex]\nabla = \hat {r} \frac {\partial}{\partial {r}} + \hat {\theta} \frac {1}{r} \frac {\partial}{\partial {\theta}} + \hat {k} \frac {\partial}{\partial {z}}[/tex]

and

[tex]V = \hat {r}V_{r} + \hat {\theta}V_{\theta} + \hat {k}V_{z}[/tex]

This is, obviously, in cylindrical coordinates.

However, I would expect the result to be as follows:

[tex]\nabla \cdot V = \frac {\partial{V_{r}}}{\partial{r}} + \frac {1}{r} \frac {\partial{V_{\theta}}}{\partial{\theta}} + \frac {\partial{V_{z}}}{\partial{z}}[/tex]

Where did I go wrong? The second two terms I get the same thing, but I am confused on where that first term comes from in the given formula. Thanks in advance.
 
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Remember that the radial and angular unit VECTORS are also functions of the angular variable. That's where your mistake lies..
 
Don't we just multiply the components in the r, theta, and z direction and add the results just like we do in the x, y, z space?
 
I do know that

[tex]\frac {\partial{\hat {r}}}{\partial{\theta}} = \hat {\theta}[/tex]

and

[tex]\frac {\partial{\hat {\theta}}}{\partial{\theta}} = - \hat {r}[/tex]

I would assume I need these, but I have no idea where to use them or exactly why.
 
Nope, here's one way of doing this:
In a slightly different notation than yours, we have:
[tex]\nabla=\vec{i}_{r}\frac{\partial}{\partial{r}}+\vec{i}_{\theta}\frac{\partial}{r\partial\theta}+\vec{i}_{z}\frac{\partial}{\partial{z}},\vec{V}=v_{r}\vec{i}_{r}+v_{\theta}\vec{i}_{\theta}+v_{z}\vec{i}_{z}[/tex]
Furthermore, we have the orthogonality relations:
[tex]\vec{i}_{r}\cdot\vec{i}_{\theta}=\vec{i}_{r}\cdot\vec{i}_{z}=\vec{i}_{\theta}\cdot\vec{i}_{z}=0[/tex]
Along with the differential relations:
[tex]\frac{\partial\vec{i}_{r}}{\partial{r}}=\frac{\partial\vec{i}_{\theta}}{\partial{r}}=\frac{\partial\vec{i}_{z}}{\partial{r}}=\frac{\partial\vec{i}_{r}}{\partial{z}}=\frac{\partial\vec{i}_{\theta}}{\partial{z}}=\frac{\partial\vec{i}_{z}}{\partial{z}}=\vec{0}[/tex]
[tex]\frac{\partial\vec{i}_{r}}{\partial\theta}=\vec{i}_{\theta},\frac{\partial\vec{i}_{\theta}}{\partial\theta}=-\vec{i}_{r},\frac{\partial\vec{i}_{z}}{\partial\theta}=\vec{0}[/tex]
Thus:
[tex]\nabla\cdot\vec{V}=\vec{i}_{r}\cdot\frac{\partial\vec{V}}{\partial{r}}+\vec{i}_{\theta}\cdot\frac{\partial\vec{V}}{r\partial\theta}+\vec{i}_{z}\cdot\frac{\partial\vec{V}}{\partial{z}}[/tex]
All that remains, is now to differentiate properly, calculate the various dot products appearing in your expression, and simplify...
 
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Why do those two have that special relation but all of the other ones are zero?

Also...why are you including the unit vectors in the dot product? I thought you just multiply the parts in the same direction and add them?


I thought the dot product was defined as:

a (dot) b = (a_x)(b_x) + (a_y)(b_y) + (a_z)(b_z) (no unit vectors here, so why are there unit vectors with cylindrical)
 
No,no,the dot product is what it is:a contracted tensor product between the 2 vectors.Vectors should be expressed in a (preferably orthonormal) basis,so that the computations should be easier...

[tex]\vec{a}\cdot\vec{b}=\left(a_{x}\vec{i}+...+a_{z}\vec{k}\right)\cdot\left(b_{x}\vec{i}+...+b_{z}\vec{k}\right)[/tex]

Daniel.
 
"Why do those two have that special relation but all of the other ones are zero?"
Because none of the unit vectors depend on "r" or "z", whereas only the radial and angular unit vectors depend on the angle.


Well, look at the Cartesian case (i.e, with [tex]\vec{V}=\vec{V}(x,y,z)[/tex]):
You can perfectly well write that in the same manner:
[tex]\nabla\cdot\vec{V}=\vec{i}_{x}\cdot\frac{\partial{\vec{V}}}{\partial{x}}+\vec{i}_{y}\cdot\frac{\partial\vec{V}}{\partial{y}}+\vec{i}_{z}\cdot\frac{\partial\vec{V}}{\partial{z}}[/tex]
We now have:
[tex]\frac{\partial\vec{V}}{\partial{x}}=\frac{\partial{v}_{x}\vec{i}_{x}}{\partial{x}}+\frac{\partial{v}_{y}\vec{i}_{y}}{\partial{x}}+\frac{\partial{v}_{z}\vec{i}_{z}}{\partial{x}}[/tex]
Now, observe the following in the Cartesian case:
1) None of the unit vectors depends on "x", that is, we have for example:
[tex]\frac{\partial{v}_{x}\vec{i}_{x}}{\partial{x}}=\frac{\partial{v}_{x}}{\partial{x}}\vec{i}_{x}[/tex]
2) [tex]\vec{i}_{x}\cdot\vec{i}_{y}=\vec{i}_{x}\cdot\vec{i}_{z}=0,\vec{i}_{x}\cdot\vec{i}_{x}=1[/tex]
Thus, we have the following simplification:
[tex]\vec{i}_{x}\cdot\frac{\partial\vec{V}}{\partial{x}}=\frac{\partial{v}_{x}}{\partial{x}}[/tex]
Similar relations hold for the y-and z derivations; thus, we regain the familiar expression:
[tex]\nabla\cdot\vec{V}=\frac{\partial{v}_{x}}{\partial{x}}+\frac{\partial{v}_{y}}{\partial{y}}+\frac{\partial{v}_{z}}{\partial{z}}[/tex]
 
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ok, ok...so I'm an idiot...I think I got it now, thanks for all the help!

One last thing though, why do the r and theta vectors depend on theta whereas all the others don't?

Obviously z would not depend on theta, and obviously theta would depend on the angle theta, but why does r depend on theta. I wouldn't think that the distance you move outwards would depend on the angle you are at?
 
  • #10
"r" does not depend on the angle, but THE RADIAL UNIT VECTOR does!
 
  • #11
The unit vector along "r" does,since it's a vector.Its modulus doesn't change as a function of angle,but its direction does...

EDIT:Mine,too.Arildno,take it easy.The shock wave that came to Belgium with the sound of your scream almost broke my window...

Daniel.
 
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  • #12
Sure, but the "outward" direction at one angle value is not PARALLELL to the "outward" direction at another angle value..

EDIT: I see a post got deleted here.
My post is an answer to that deleted post.
 
  • #13
Isn't the unit r vector just in the outward direction from the z axis though? I realize that in x-y-z coordinates that the r vector would change with changing theta, but cylindrical coords are different

EDIT: No, you just looked like a mind reader because it was a response to this post (which was deleted then reposted with different wording) :smile:
 
Last edited:
  • #14
errr...um ok...I guess i'll just have to try thinking about it some more...anyways thanks for the help guys!
 

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