Simple cylindrical coords problem

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Discussion Overview

The discussion revolves around a problem involving a rigid body rotating about a fixed axis with a constant angular velocity $\omega$ along the z-axis. Participants are tasked with expressing the position vector in cylindrical coordinates and calculating the velocity vector and the curl of the velocity vector. The focus is on the mathematical formulation and notation used in the calculations.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • Participants express the position vector as $\vec{r} = \vec{\rho}\rho + \vec{z}z$ and calculate the velocity vector as $\vec{v} = \omega \times \vec{r}$.
  • There is a question regarding the notation used in the solution, specifically whether the result should include the unit vector $\hat{\phi}$.
  • Participants note that the curl of the velocity vector is calculated using the appropriate notation for the gradient operator, leading to confusion about the expected answer in the book.
  • One participant suggests that the book may contain a typo regarding the inclusion of the unit vector in the answer for part (a) and the direction in part (b).
  • Another participant confirms the calculation of the curl and discusses the importance of including vector components in the final answer.

Areas of Agreement / Disagreement

There is no consensus on whether the book's answers contain typos, as participants express differing views on the correctness of their own calculations versus the book's solutions. The discussion remains unresolved regarding the accuracy of the book's answers.

Contextual Notes

Participants express uncertainty about the notation and the expected format of the answers, particularly regarding the inclusion of unit vectors and vector components in the curl calculation.

ognik
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Rigid body rotating about a fixed axis with constant $\omega$ along the z axis. Express position vector $\vec{r}$ in cyl. circ. cords and using cyl. circ. cords find (a) $\vec{v}=\omega \times \vec{r}$ (b) $\nabla \times \vec{v}$

So $ \vec{r} = \vec{\rho}\rho + \vec{z}z $

(a) = $\begin{vmatrix}
\hat{\rho}&\hat{\phi}&\hat{z}\\0&0&\omega\\\ \rho&\ 0&z
\end{vmatrix} = \vec{\phi}\omega \rho $

But the solution shown is $ \vec{\phi} \omega \rho $? Shouldn't it be the unit vector $\hat{\phi}$?

(b) $ \nabla = \left( \partial_{\rho}, \frac{1}{\rho} \partial_{\phi}, \partial_z \right) $

$ \therefore \nabla \times \vec{v} =
\begin{vmatrix}
\hat{\rho}&\hat{\phi}&\hat{z}\\\partial_{\rho}, & \frac{1}{\rho} \partial_{\phi}, &\partial_z \\\ 0&\ \omega \rho & 0
\end{vmatrix}$
which is obviously not going to give me the answer in the book ($2\omega$), so what am I missing please? Also isn't the book's answer missing a direction?
 
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ognik said:
Rigid body rotating about a fixed axis with constant $\omega$ along the z axis. Express position vector $\vec{r}$ in cyl. circ. cords and using cyl. circ. cords find (a) $\vec{v}=\omega \times \vec{r}$ (b) $\nabla \times \vec{v}$

So $ \vec{r} = \vec{\rho}\rho + \vec{z}z $

(a) = $\begin{vmatrix}
\hat{\rho}&\hat{\phi}&\hat{z}\\0&0&\omega\\\ \rho&\ 0&z
\end{vmatrix} = \vec{\phi}\omega \rho $

But the solution shown is $ \vec{\phi} \omega \rho $? Shouldn't it be the unit vector $\hat{\phi}$?

(b) $ \nabla = \left( \partial_{\rho}, \frac{1}{\rho} \partial_{\phi}, \partial_z \right) $

$ \therefore \nabla \times \vec{v} =
\begin{vmatrix}
\hat{\rho}&\hat{\phi}&\hat{z}\\\partial_{\rho}, & \frac{1}{\rho} \partial_{\phi}, &\partial_z \\\ 0&\ \omega \rho & 0
\end{vmatrix}$
which is obviously not going to give me the answer in the book ($2\omega$), so what am I missing please? Also isn't the book's answer missing a direction?

Hi ognik,

I am not sure what your problem is with the first part. The solution you have obtained; $\vec{\phi} \omega \rho $ seems to be correct.

For the second part the notation $\nabla \times \vec{v}$ seems to indicate you have to find the Curl of $\vec{v}$ not the gradient.
 
Hi, thanks - must be a typo in the book for part a, left out the \hat, good to have confirmation.

Part b - oops, yes curl, which should be: $\frac{1}{\rho}\begin{vmatrix}
\hat{\rho}&\rho\hat{\phi}&\hat{z}\\ \partial_{\rho}&\partial_{\phi}&\partial_z \ \\0&\rho \omega \rho &0
\end{vmatrix}$ for $ \vec{v}=\hat{\phi}\omega \rho $

I get $ \nabla \times \vec{v} = \hat{z}2\omega $, the book again appears to have a typo - no $\hat{z}$, assume mine is OK? Thanks for the help.
 
ognik said:
Hi, thanks - must be a typo in the book for part a, left out the \hat, good to have confirmation.

Part b - oops, yes curl, which should be: $\frac{1}{\rho}\begin{vmatrix}
\hat{\rho}&\rho\hat{\phi}&\hat{z}\\ \partial_{\rho}&\partial_{\phi}&\partial_z \ \\0&\rho \omega \rho &0
\end{vmatrix}$ for $ \vec{v}=\hat{\phi}\omega \rho $

I get $ \nabla \times \vec{v} = \hat{z}2\omega $, the book again appears to have a typo - no $\hat{z}$, assume mine is OK? Thanks for the help.

Well, the Curl should always be a vector. If the book only asks for the magnitude of Curl the answer is $2\omega$ otherwise the vector component should be included. :)
 

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