Triple Integration: Transform Equation to Spherical Coordinates

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SUMMARY

The discussion focuses on transforming an integral equation from Cartesian coordinates to spherical coordinates, specifically for calculating the electric field generated by a Gaussian charge distribution. The integral involves the position vectors \(\vec{x}\), \(\vec{x'}\), and \(\vec{x_0}\), with the volume element expressed as \(d^3x' = dx'~dy'~dz'\). Participants clarify that the integration limits extend to infinity and suggest using the potential \(\phi\) for easier integration, leading to the expression \(\vec{E}(\vec{x}) = -\nabla \phi(\vec{x})\).

PREREQUISITES
  • Understanding of vector calculus, particularly gradient and divergence operations.
  • Familiarity with Gaussian functions and their properties.
  • Knowledge of electric field concepts and charge distributions.
  • Proficiency in changing coordinate systems, specifically from Cartesian to spherical coordinates.
NEXT STEPS
  • Study the derivation of electric fields from charge distributions using integral calculus.
  • Learn about spherical coordinates and their application in vector calculus.
  • Explore the properties of Gaussian functions and their role in physics.
  • Investigate techniques for simplifying integrals involving vector fields.
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Students and professionals in physics, particularly those focusing on electromagnetism and mathematical methods in physics, will benefit from this discussion.

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Homework Statement


Transform the equation from cartesians coordinates to spherical coordinates.


Homework Equations


[tex]\int_\infty\int_\infty\int_\infty<br /> exp\left\{<br /> \frac{-\left| \vec{x'}-\vec{x}_0 \right|^2}{2 \sigma}<br /> \right\}<br /> \frac{\left( \vec{x} - \vec{x'} \right)}{\left| \vec{x} - \vec{x'} \right|^{3}} d^3x'[/tex]


The Attempt at a Solution


I'm confused by the [tex]\vec{x}[/tex], [tex]\vec{x'}[/tex] and [tex]\vec{x}_0[/tex]... I know it can be done: nothing depends on the angle here, so I should just get something depending on [tex]\vec{r}[/tex].

Thank you for any hints...
 
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I'm equally confused by your integrand expression. It's supposed to be dxdydz isn't it? And what are the limits of your integration? And what does x' mean as both a scalar variable or vector function variable?
 
Hi Defennder, thanks for your reply.

Yes, [tex]d^3x'[/tex] is indeed [tex]dx'~dy'~dz'[/tex]: a volume element.

The integration is over infinity.

[tex]\vec{x'}[/tex] is the integration variable. It is a position vector [tex](x',y',z')[/tex].

Maybe I'll explain more the problem...

The integral is the electric field at position [tex]\vec{x}[/tex], caused by a charge distribution of gaussian shape:
[tex]\vec{E}\left(\vec{x}\right) = <br /> k \int_{x'=-\infty}^{\infty} \int_{y'=-\infty}^{\infty} \int_{z'=-\infty}^{\infty}<br /> \rho\left(\vec{x'}\right) \frac{\vec{x} - \vec{x'}}{\left| \vec{x} - \vec{x}'\right|^3} ~dx'~dy'~dz'[/tex]
[tex] \rho\left(\vec{x}\right) & = & \rho_0 \exp\left(<br /> -\frac{\left(\vec{x} - \vec{x_0}\right)^2}{2 \sigma^2}<br /> \right)[/tex]
where:
[tex]\vec{x}[/tex] is the position where the field is wanted;
[tex]\vec{x'}[/tex] is the integration variable;
[tex]\vec{x_0}[/tex] is the particle center;
[tex]\sigma[/tex] is the particle width.

I think I'll use the potential instead, for an easier integration:
[tex]\vec{E}\left(\vec{x}\right) = - \nabla \phi\left(\vec{x}\right)[/tex]
[tex] \phi\left(\vec{x}\right) = <br /> k \int_{x'=-\infty}^{\infty} \int_{y'=-\infty}^{\infty} \int_{z'=-\infty}^{\infty}<br /> \rho\left(\vec{x'}\right) \frac{1}{\left| \vec{x} - \vec{x}'\right|} ~dx'~dy'~dz'[/tex]

I've done a variable change for [tex]\vec{x} - \vec{x}'[/tex] but then I'm stuck in the gaussian...

Thanx for any hints.

(Sorry if any mistakes have slipped, I'm writting this from memory and it's getting late...)
 

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