EM: Gauss' law for electricity

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SUMMARY

The discussion focuses on applying Gauss' law to determine the electric field strength at the surface of a solid sphere with a non-uniform volume charge density defined as \(\rho = \rho_0 e^{r/R}\). The initial attempt incorrectly assumed a uniform charge distribution, leading to an erroneous calculation of the enclosed charge. The correct approach requires integrating the charge density over the sphere's volume to accurately compute the total charge, ultimately yielding the correct expression for the electric field strength at the surface.

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Homework Statement



A solid sphere of radius R carries a volume charge density [tex]\rho = \rho_0e^{r/R}[/tex], where [tex]\rho_0[/tex] is a constant and r is the distance from the center.

Find an expression for the electric field strength at the sphere's surface.

Homework Equations



[tex]\int\vec{E}.d\vec{A} = \frac{q}{\epsilon_0}[/tex]

The Attempt at a Solution


[tex]E * 4 \pi R^2= \frac{\rho \frac{4}{3}\pi R^3}{\epsilon_0} = \frac{\rho_0e \frac{4}{3}\pi R^3}{\epsilon_0} = \frac{\rho_0 e R}{3*\epsilon_0}[/tex]

This is not correct. Why not? With the gaussian surface right at the sphere's surface, the enclosed charge is the volume charge density times the volume, no? What am I missing?
 
Last edited:
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The charge density is not uniform; it varies with radius r within the sphere. You must integrate the density over the sphere's volume to calculate the total charge.
 
Can't believe I missed that. Thanks, got the correct solution now.
 

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