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A spherically symmetric charged distribution has a charged density given by ρ = a / r, where a is a constant. Find the field within the sphere as a function of r. [

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Answer:

Electric field,
E = (a)/(2epsilon)

Given:

charge density,
\rho = (a)/(r)

a = constant

Solution:

Area of sphere =
4\pi r_(2) dr

Small charge dq on a sphere of thickness r is:

dq =
\rho * A* dr

dq =
4\rho \pi r_(2) dr (1)

Integrating both the sides, we get:


dq = 4\rho \pi r_(2) dr


\int dq = \int (a)/(r)* 4\pi r^(2) dr


q(r)= 2\pi r^(2)a - 0 = 2\pi r^(2)a

Therefore, the total charge enclosed by a sphere of radius r is
q(r)= 2\pi r^(2)a

Now, by Gauss Law, flux emerging out of the surface is equal to
(1)/(\epsilon_(o)) times the total charge enclosed:


A* E = (q)/(\epsilon_(o))


4\pi r^(2)* E = \frac{}{\epsilon_(o)}


E = (2\pi r^(2)a)/(\epsilon_(o))


E = (a)/(2epsilon)

where

E = electric field

User Hui Zheng
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