How to derive the spherical coordinate form for Laplacian

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Homework Help Overview

The discussion revolves around deriving the spherical coordinate form for the Laplacian operator, specifically focusing on the mathematical expressions and transformations involved in the process.

Discussion Character

  • Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the necessity of using the chain rule for coordinate transformations and express uncertainty about the next steps after establishing the coordinate relationships. There is mention of writing derivatives in terms of polar coordinates and the suggestion to explore polar or cylindrical coordinates first for clarity.

Discussion Status

Some guidance has been provided regarding the use of the chain rule and the need for coordinate transformations. Participants are exploring different approaches, but no consensus has been reached on a specific method or solution.

Contextual Notes

There is an indication that the problem may involve tedious calculations and that participants are working with fundamental relationships between Cartesian and spherical coordinates.

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Homework Statement



[tex]\Delta f = \frac{1}{{r^2 }}\frac{\partial }{{\partial r}}\left( {r^2 \frac{{\partial f}}{{\partial r}}} \right) + \frac{1}{{r^2 \sin \phi }}\frac{\partial }{{\partial \phi }}\left( {\sin \phi \frac{{\partial f}}{{\partial \phi }}} \right) + \frac{1}{{r^2 \sin ^2 \phi }}\frac{{\partial ^2 f}}{{\partial \theta ^2 }}[/tex]



Homework Equations




[tex]\nabla ^2 = \frac{{\partial ^2 }}{{\partial x^2 }} + \frac{{\partial ^2 }}{{\partial y^2 }} + \frac{{\partial ^2 }}{{\partial y^2 }}[/tex]

The Attempt at a Solution

 
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What have you attempted so far?
 
I have just attmpted to write the coordinate change:x=r sin([tex]\theta[/tex])cos([tex]\phi[/tex]) y=rsin([tex]\theta[/tex])sin([tex]\phi[/tex]) z=rcos([tex]\theta[/tex])

I don't know what to do next.
 
Just use the chain rule, repeatedly. Nothing very deep but labor intensive and tedious!

[tex]\frac{\partial f}{\partial x}= \frac{\partial f}{\partial r}\frac{\partial r}{\partial x}+ \frac{\partial f}{\partial \theta}\frac{\partial \theta}{\partial x}+ \frac{\partial f}{\partial \phi}\frac{\partial \phi}{\partial x}[/tex]

You will need the coordinate equations, "the other way around":
[tex]r= (x^2+ y^2+ z^2)^{1/2}[/tex]
[tex]\phi= arctan(\frac{y}{x})[/tex]
[tex]\theta= arctan(\frac{\sqrt{x^2+ y^2}}{z}[/tex]
and you will want to write the derivatives in terms of the polar coordinates:
[tex]\frac{d\phi}{dx}= \frac{1}{1+ \frac{y^2}{x^2}}\left(-\frac{y}{x^2}\right)[/tex]
and, multiplying numerator and denominator by [itex]x^2[/itex],
[tex]= \frac{-y}{x^2+ y^2}= -\frac{r sin(\phi)}{r^2 sin^2(\theta)}= -\frac{sin(\phi)}{r sin^2(\theta)}[/tex].

If you haven't done it already, I recommend doing polar or cylindrical coordinates first to get the idea.
 
HallsofIvy said:
Just use the chain rule, repeatedly. Nothing very deep but labor intensive and tedious!

[tex]\frac{\partial f}{\partial x}= \frac{\partial f}{\partial r}\frac{\partial r}{\partial x}+ \frac{\partial f}{\partial \theta}\frac{\partial \theta}{\partial x}+ \frac{\partial f}{\partial \phi}\frac{\partial \phi}{\partial x}[/tex]

You will need the coordinate equations, "the other way around":
[tex]r= (x^2+ y^2+ z^2)^{1/2}[/tex]
[tex]\phi= arctan(\frac{y}{x})[/tex]
[tex]\theta= arctan(\frac{\sqrt{x^2+ y^2}}{z}[/tex]
and you will want to write the derivatives in terms of the polar coordinates:
[tex]\frac{d\phi}{dx}= \frac{1}{1+ \frac{y^2}{x^2}}\left(-\frac{y}{x^2}\right)[/tex]
and, multiplying numerator and denominator by [itex]x^2[/itex],
[tex]= \frac{-y}{x^2+ y^2}= -\frac{r sin(\phi)}{r^2 sin^2(\theta)}= -\frac{sin(\phi)}{r sin^2(\theta)}[/tex].

If you haven't done it already, I recommend doing polar or cylindrical coordinates first to get the idea.

Thank you very much,I see
 

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