
Stephen K. answered 09/16/14
Tutor
4.9
(798)
Physics PhD experienced in teaching undergraduates
Dalia,
For this problem you need to consider two scenarios, (1) inside the sphere and (2) outside the sphere as separate problems.
Start with the general expression for the electric field:
E = kq/r².
We can then write that dE/dq = k/r² or dE = kdq/r²
However, we're not given q, we're given the charge density ρ. The amount of charge enclosed by a portion of the sphere is then:
qenclosed = ρ·(4/3)πr³ , since the amount of charge enclosed depends only on r ⇒
dq = (4/3)πρr²dr
Substituting into the expression for dE: dE = (k/r²)(4/3)(πρr²)dr
r² in the numerator cancels with r² in the denominator, so:
E = 4πkρ∫dr, evaluated from r = 0 to r, which leaves us with:
(a) Er = (4/3)πkρr , for r < a
for part (b) we start by noting that all of the charge Q resides inside the sphere when r > a.
Then Q = ρ·(4/3)πa³
Then for Er when r > a
E = kQ/r² which is simply the field of a point charge.
To put this back in terms of ρ and a just substitute for Q
(b) Er = 4πkρa³/3r² , r > a