Advanced Gauss's Law Question

blackhawk97
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A solid sphere of radius R has a non-uniform volume charge density \rho(r) and a constant surface charge density \sigma. If the field inside the sphere is uniform and radially atuned, and the field a distance 2R away from the center is zero, find \rho and \sigma in terms of R, r (distance from the center of the sphere), and Q_\text{volume} (the charge associated with \rho, but not with \sigma).

Homework Equations


Gauss's Law

The Attempt at a Solution


I'm not sure how to proceed, but I think the solution should begin by find the total charge on the sphere (ie., adding the integral of the charge calculable from the surface charge density with the integral of the charge calculable from the volume charge density). Am I on the right track?
 
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So, inside the sphere, what does Gauss's law say? Outside the sphere? Try drawing Gaussian surfaces which are spheres inside and outside the sphere of charge.
 
I know how to do the first part, i think... (finding \sigma). Basically you just use Gauss's Law

\oint{E \cdot dA}=\frac{Q_\text{enclosed}}{\epsilon_0}

... except you set the r in that equation equal to 2R, so you can ultimately set the expression for the E-field equal to zero and... yeah.

But the part about \rho still has me stumped. Can anyone offer a bit more help?

Also, correction to the problem: the field inside the sphere is not radially atuned, it is directed radially outwards.
 
So can you express \sigma in terms of Q_{total}?

For the \rho part you have to take Gauss surfaces inside the sphere as Matterwave said.
 
To solve this, I first used the units to work out that a= m* a/m, i.e. t=z/λ. This would allow you to determine the time duration within an interval section by section and then add this to the previous ones to obtain the age of the respective layer. However, this would require a constant thickness per year for each interval. However, since this is most likely not the case, my next consideration was that the age must be the integral of a 1/λ(z) function, which I cannot model.
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