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...)