It's Gaussy time.

A ball of radius R R is charged with a volume charge density which with the distance r r from the centre as ρ = α r 2 \rho = \alpha r^2 where α \alpha is a positive constant. The magnitude of electric field intensity at a distance r = R 2 r = \dfrac{R}{2} is given by:

E = a α R 3 b ϵ 0 \large E = \dfrac{a \alpha R^3}{b \epsilon_0}

a a and b b are co-prime.

What is a + b ? a+b \ ?


The answer is 41.

This section requires Javascript.
You are seeing this because something didn't load right. We suggest you, (a) try refreshing the page, (b) enabling javascript if it is disabled on your browser and, finally, (c) loading the non-javascript version of this page . We're sorry about the hassle.

1 solution

Consider a thin spherical shell as an element of arbitrary radius x x and thickness d x dx .

Let d q dq be the charge associated with that shell and is given by

d q = ρ α x 2 × 4 π x 2 d x dq = \rho \alpha x^2 \times 4 \pi x^2 dx

q = 0 R / 2 d q = q e n c l o s e d \Rightarrow q = \displaystyle \int_{0}^{R/2} dq = q_{enclosed}

By Gauss' Law,

E × 4 π ( R 2 ) 2 = q e n c l o s e d ϵ 0 E \times 4 \pi (\dfrac{R}{2})^2 = \dfrac{q_{enclosed}}{\epsilon_0}

E = α R 3 40 ϵ 0 E = \boxed{\dfrac{\alpha R^3}{40\epsilon_0}}

a + b = 41 a+b = 41

0 pending reports

×

Problem Loading...

Note Loading...

Set Loading...