Conversion from Cartesian to Cylindrical Coordinates

[seaspecies]

Hello.

I am interested in learning the mathematical derivation from Cartesian coordinates Navier-Stokes equation to cylindrical coordinates Navier-Stokes equation. These equations have similar forms to the basic heat and mass transfer differential governing equations. I’ve tried looking online and at a variety of fluid mechanics books and heat transfer books and they all simply skip the math and go straight into just stating the equations. It seems like it is too complicated that it is not worth saying. Or it might be so trivial that I might be missing something. Maybe it is not worth it but I am curious of how it is done.

I attached the part the I am most confused about as a jpeg. How do they equal?

$$\frac{\partial T^2}{\partial x^2}+\frac{\partial T^2}{\partial y^2}=\frac{1}{r}\frac{\partial}{\partial r}r\frac{\partial T}{\partial r}+\frac{1}{r^2}\frac{\partial T^2}{\partial\theta^2}<br />$$

Thanks. I am sorry if I had any errors I am new here.

 

[seaspecies]

So I've attached how far I've gotten but I am not sure if there are any tricks because I'm stuck.

$$\frac{\partial }{\partial x}=\frac{\partial }{\partial r}\frac{\partial r}{\partial x}=\frac{\partial }{\partial r}cos\theta$$

$$\frac{\partial }{\partial y}=\frac{\partial }{\partial r}\frac{\partial r}{\partial y}=\frac{\partial }{\partial r}sin\theta$$

$$\frac{\partial T}{\partial x}=\frac{\partial r}{\partial x}\frac{\partial T}{\partial r} = cos\theta\frac{\partial T}{\partial r}$$

$$\frac{\partial T}{\partial y}=\frac{\partial r}{\partial y}\frac{\partial T}{\partial r} = sin\theta\frac{\partial T}{\partial r}$$

$$\frac{\partial T^2}{\partial x^2}+\frac{\partial T^2}{\partial y^2} = <br /> sin\theta \frac{\partial }{\partial r} (sin\theta \frac{\partial T}{\partial r}) + cos\theta \frac{\partial }{\partial r} (cos\theta\frac{\partial T}{\partial r}) =? \frac{1}{r}\frac{\partial }{\partial r}r\frac{\partial T}{\partial r}+\frac{1}{r^2}\frac{\partial T^2}{\partial \theta^2}$$** Edited so that LaTex would work. (I just figured it out )
on a side note, I am not sure if this warrents a new topic, but I see my engineering colleagues interchange d and $$\partial$$. I believe there is a difference mathamatically but what is it in particular and will it change the meaning the governing equations mathamatically?

 

[arildno]

Well, usually, the topic of coordinate transformations would be taught in courses of vector analysis.
It is not particularly complicated (it should be easily understood), but the arithmetic can be quite messy if we wish to keep the notation on an intuitively clear level. Do you have a vector analysis textbook?

 

[HallsofIvy]

Basically, changeing derivatives from one coordinate system to another is careful application of the chain rule.

Your
$$\frac{\partial }{\partial x}=\frac{\partial }{\partial r}\frac{\partial r}{\partial x}=\frac{\partial }{\partial r}cos\theta$$
is only partially correct.
Since in polar coordinates, x depends on two variables, r and $\theta$,
$$\frac{\partial \phi}{\partial x}= \frac{\partial r}{\partial x}\frac{\partial \phi}{\partial r}+ \frac{\partial \theta}{\partial x} \frac{\partial \phi}{\partial \theta}$$

[tex]r= \sqrt{x^2+ y^2}= \left(x^2+ y^2\right)^{\frac{1}{2}}[/itex] so <br /> $$\frac{\partial r}{\partial x}= \frac{1}{2}\left(x^2+ y^2\right)^{-\frac{1}{2}}\left(2x\right)= \frac{x}{\sqrt{x^2+ y^2}}= \frac{r cos(\theta)}{r}= cos(\theta)$$<br /> <br /> Okay, now I see where you got your expression above- but it isn't complete.<br /> <br /> [tex]\theta= tan^{-1}\frac{y}{x}[/itex] <br /> so<br /> [tex]\frac{\partial \theta}{\partial x}= \frac{1}{1+ \frac{y^2}{x^2}}\left(-\frac{y}{x^2}\right)= \frac{-y}{x^2+ y^2}= \frac{-r sin(\theta)}{r^2}= -\frac{1}{r}sin(\theta)[/itex]<br /> <br /> That gives<br /> $$\frac{\partial \phi}{\partial x}= cos(\theta)\frac{\partial \phi}{\partial r}- \frac{1}{r}sin(\theta)\frac{\partial \phi}{\partial \theta}$$<br /> <br /> Once again, it really just the chain rule, <b>carefully</b> applied.<br /> <br /> Now, make sure you have plenty of time and paper, take a deep breath, and do it again to find $\frac{\partial^2 \phi}{\partial x^2}$![/tex][/tex][/tex]

 

[seaspecies]

Question

Hello. Thanks for the reply. I am wondering if this is mathematically viable:
Assuming:
$$\frac{\partial \phi}{\partial x}= \frac{\partial r}{\partial x}\frac{\partial \phi}{\partial r}+ \frac{\partial \theta}{\partial x} \frac{\partial \phi}{\partial \theta}$$ (1)

and

Assuming:
$$\frac{\partial}{\partial x}= \frac{\partial r}{\partial x}\frac{\partial}{\partial r}+ \frac{\partial \theta}{\partial x} \frac{\partial}{\partial \theta}$$ (2)

Would the following work?
$$\frac{\partial^2 \phi}{\partial x^2} = \frac{\partial}{\partial x}\frac{\partial \phi}{\partial x}$$ (3)

Plugging equation 1 and 2 into equation 3.$$\frac{\partial^2 \phi}{\partial x^2} = (\frac{\partial r}{\partial x}\frac{\partial}{\partial r}+ \frac{\partial \theta}{\partial x} \frac{\partial}{\partial \theta}) (\frac{\partial r}{\partial x}\frac{\partial \phi}{\partial r}+ \frac{\partial \theta}{\partial x} \frac{\partial \phi}{\partial \theta})$$

$$\frac{\partial^2 \phi}{\partial x^2} = <br /> <br /> \frac{\partial r}{\partial x}\frac{\partial}{\partial r}<br /> \frac{\partial r}{\partial x}\frac{\partial \phi}{\partial r}<br /> +<br /> \frac{\partial r}{\partial x}\frac{\partial}{\partial r}<br /> \frac{\partial \theta}{\partial x} \frac{\partial \phi}{\partial \theta}<br /> +<br /> \frac{\partial \theta}{\partial x}\frac{\partial}{\partial \theta}<br /> \frac{\partial r}{\partial x}\frac{\partial \phi}{\partial r}<br /> +<br /> \frac{\partial \theta}{\partial x}\frac{\partial}{\partial \theta}<br /> \frac{\partial \theta}{\partial x} \frac{\partial \phi}{\partial \theta}<br />$$

$$\frac{\partial^2 \phi}{\partial x^2} + \frac{\partial^2 \phi}{\partial y^2} = <br /> <br /> \frac{\partial r}{\partial x}\frac{\partial}{\partial r}<br /> \frac{\partial r}{\partial x}\frac{\partial \phi}{\partial r}<br /> +<br /> \frac{\partial r}{\partial x}\frac{\partial}{\partial r}<br /> \frac{\partial \theta}{\partial x} \frac{\partial \phi}{\partial \theta}<br /> +<br /> \frac{\partial \theta}{\partial x}\frac{\partial}{\partial \theta}<br /> \frac{\partial r}{\partial x}\frac{\partial \phi}{\partial r}<br /> +<br /> \frac{\partial \theta}{\partial x}\frac{\partial}{\partial \theta}<br /> \frac{\partial \theta}{\partial x} \frac{\partial \phi}{\partial \theta}<br /> <br /> +<br /> <br /> \frac{\partial r}{\partial y}\frac{\partial}{\partial r}<br /> \frac{\partial r}{\partial y}\frac{\partial \phi}{\partial r}<br /> +<br /> \frac{\partial r}{\partial y}\frac{\partial}{\partial r}<br /> \frac{\partial \theta}{\partial y} \frac{\partial \phi}{\partial \theta}<br /> +<br /> \frac{\partial \theta}{\partial y}\frac{\partial}{\partial \theta}<br /> \frac{\partial r}{\partial y}\frac{\partial \phi}{\partial r}<br /> +<br /> \frac{\partial \theta}{\partial y}\frac{\partial}{\partial \theta}<br /> \frac{\partial \theta}{\partial y} \frac{\partial \phi}{\partial \theta}$$

The
$$\frac{\partial}{\partial \theta}\frac{\partial \phi}{\partial r}$$
terms and its other combinations cancel out algebraically leaving only four terms

$$\frac{\partial^2 \phi}{\partial x^2} + \frac{\partial^2 \phi}{\partial y^2} = <br /> <br /> \frac{\partial r}{\partial x}\frac{\partial}{\partial r}<br /> \frac{\partial r}{\partial x}\frac{\partial \phi}{\partial r}<br /> +<br /> \frac{\partial \theta}{\partial x}\frac{\partial}{\partial \theta}<br /> \frac{\partial \theta}{\partial x} \frac{\partial \phi}{\partial \theta}<br /> <br /> +<br /> <br /> \frac{\partial r}{\partial y}\frac{\partial}{\partial r}<br /> \frac{\partial r}{\partial y}\frac{\partial \phi}{\partial r}<br /> +<br /> \frac{\partial \theta}{\partial y}\frac{\partial}{\partial \theta}<br /> \frac{\partial \theta}{\partial y} \frac{\partial \phi}{\partial \theta}$$If this works, ultimately I get something like this which is so close but I can’t get rid of the sin and cos (4 of the 8 terms cancel out and 2 of the terms could be combined leaving only 3 terms left). Is there a mathamatical identity or any way to approach this?

$$sin\theta\frac{\partial}{\partial r} sin\theta\frac{\partial\phi}{\partial r} + cos\theta\frac{\partial}{\partial r} cos\theta\frac{\partial\phi}{\partial r} + \frac{1}{r^2}\frac{\partial^2 \phi}{\partial\theta^2}$$

which should ultimately equal the following if everything turns out well?

$$\frac{1}{r}\frac{\partial }{\partial r}r\frac{\partial \phi}{\partial r}+\frac{1}{r^2}\frac{\partial \phi^2}{\partial \theta^2}$$Appendix:
$$\frac{\partial r}{\partial x}= \frac{1}{2}\left(x^2+ y^2\right)^{-\frac{1}{2}}\left(2x\right)= \frac{x}{\sqrt{x^2+ y^2}}= \frac{r cos(\theta)}{r}= cos(\theta)$$

$$\frac{\partial r}{\partial y}= \frac{1}{2}\left(x^2+ y^2\right)^{-\frac{1}{2}}\left(2y\right)= \frac{y}{\sqrt{x^2+ y^2}}= \frac{r sin(\theta)}{r}= sin(\theta)$$

 

[arildno]

No.
Understand what the symbols mean, before spewing them out.

 

[seaspecies]

Dear Arildno, I am sorry for the confusion. I tried add more text and equations to show my logical flow. Thanks for your reply.

Dear HallsOfIvy, Thanks! It makes much more sense now. I am wonder if my method was what you meant by:
"Now, make sure you have plenty of time and paper, take a deep breath, and do it again"

If my last method would not work did you want me to take the following approach
$$\frac{\partial^2\phi}{\partial x^2}=\frac{\partial^2 r}{\partial x^2}\frac{\partial^2\phi}{\partial r^2}<br /> <br /> + \frac{\partial^2 \theta}{\partial x^2}\frac{\partial^2\phi}{\partial r^2}$$

And compute all the second derivatives. But then my final answer won't have a
$$\frac{\partial }{\partial r}r\frac{\partial \phi}{\partial r}$$

Thanks!

 

[arildno]

I'm sorry about my previous reply, here's how you migth do it:
We have the 2-D Laplacian:
$$\nabla^{2}\phi=\frac{\partial^{2}\phi}{\partial{x}^{2}}+\frac{\partial^{2}\phi}{\partial{y}^{2}},\nabla^{2}\equiv\nabla\cdot\nabla,\nabla=\vec{i}\frac{\partial}{\partial{x}}+\vec{j}\frac{\partial}{\partial{y}}$$

If we write the gradient operator $\nabla$ in terms of 2-D polar coordinates, we have:
[tex]\nabla=\vec{i}_{r}\frac{\partial}{\partial{r}}+\vec{i}_{\theta}\frac{\partial}{r\partial\theta}[/itex]<br /> <br /> Notice that the unit vectors varies with the angle (but not with the radius!); we have:<br /> $$\frac{\partial\vec{i}_{r}}{\partial\theta}=\vec{i}_{\theta},\frac{\partial\vec{i}_{\theta}}{\partial\theta}=-\vec{i}_{r}$$<br /> <br /> Now, perform the dot product $\nabla\cdot\nabla$:<br /> $$\nabla^{2}\equiv\nabla\cdot\nabla=\vec{i}_{r}\cdot\frac{\partial}{\partial{r}}(\vec{i}_{r}\frac{\partial}{\partial{r}}+\vec{i}_{\theta}\frac{\partial}{r\partial\theta})+\frac{1}{r}\vec{i}_{\theta}\cdot\frac{\partial}{\partial\theta}(\vec{i}_{r}\frac{\partial}{\partial{r}}+\vec{i}_{\theta}\frac{\partial}{r\partial\theta})$$<br /> <br /> By applying the product rules of differentiation, remembering that the unit vectors are constant with respect with r and that $\vec{i}_{r}\cdot\vec{i}_{\theta}=0$, we end up with:<br /> $$\nabla^{2}=\frac{\partial^{2}}{\partial{r}^{2}}+\frac{1}{r}\frac{\partial}{\partial{r}}+\frac{1}{r^{2}}\frac{\partial^{2}}{\partial\theta^{2}}=\frac{1}{r}\frac{\partial}{\partial{r}}(r\frac{\partial}{\partial{r}})+\frac{1}{r^{2}}}}\frac{\partial^{2}}{\partial\theta^{2}}$$<br /> This is the desired repesentation of the Laplacian operator in polar coordinates.[/tex]

 

[seaspecies]

Dear arildno,

Thanks! It makes much more sense now. I had to look back onto my old texts but I've got it figured out. Yet I am alittle confused on the last part. I tried figuring it out but I could not figure out how to combine the two terms into one:

$$\frac{\partial^{2}}{\partial{r}^{2}}+\frac{1}{r}\frac{\partial}{\partial{r}}=\frac{1}{r}\frac{\partial}{\partial{r}}(r\frac{\partial}{\partial{r}})$$

$$\nabla^{2}=\frac{\partial^{2}}{\partial{r}^{2}}+\frac{1}{r}\frac{\partial}{\partial{r}}+\frac{1}{r^{2}}\frac{\partial^{2}}{\partial\theta^{2}}=\frac{1}{r}\frac{\partial}{\partial{r}}(r\frac{\partial}{\partial{r}})+\frac{1}{r^{2}}}}\frac{\partial^{2}}{\partial\theta^{2}}$$

Thanks

 

[arildno]

Well:
$$\frac{\partial}{\partial{r}}(r\frac{\partial}{\partial{r}})=\frac{\partial{r}}{\partial{r}}\frac{\partial}{\partial{r}}+r\frac{\partial}{\partial{r}}(\frac{\partial}{\partial{r}})=\frac{\partial}{\partial{r}}+r\frac{\partial^{2}}{\partial{r}^{2}}$$

 

[seaspecies]

Thanks! It all makes sense now. It was so simple I didn't see it. Thanks again!

 

[arildno]

My pleasure!

 

[luckyyy]

Hi Sir...

what about this...i could not understand about ur conversion from cartisian to cylinrical coordinate, becoz it has a lot of mistakes, ...please tell me the true method...

 

[cristo]

what about this...i could not understand about ur conversion from cartisian to cylinrical coordinate, becoz it has a lot of mistakes, ...please tell me the true method...

What do you mean? Please make your request more specific; state an exact question and the work you have done towards it.

 

[luckyyy]

Luckyyy

i think, i did wrong something...but i am very interesting to solution of this, i spent many time to solve this but i could't...