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Question: A solid non-conducting sphere of radius \(R\), having a spherical cavity of radius \(\dfrac{R}{2}\) ...

A solid non-conducting sphere of radius RR, having a spherical cavity of radius R2\dfrac{R}{2} as shown, carries a uniformly distributed charge qq. The electric field at the centre of the cavity is:

Explanation

Solution

From the Gauss Law of Electrostatics we can find out the electric field.The electric field inside a non-conducting sphere is 00. So, we have to find out the electric field only of the cavity. The electric field of the cavity is the same as the electric field at the surface of any sphere. Since, the cavity is in the positive direction of the X-axis so we will consider the outcome to be a positive value.

Complete step by step answer:
From the Gauss Law of Electrostatics we know,
E.dS=qε0(1)\oint {E.dS} = \dfrac{q}{{{\varepsilon _0}}} - - - - - \left( 1 \right) where EE is the electric field, dSdS is the enclosed surface area, qq is the charge enclosed.

In the given figure O is the centre. Let AA be any point on the surface. The charge enclosed in the non-conducting sphere is=0 = 0. So, the electric field here is also 00. We have to just find out the electric field of the cavity. According to the given question,
Charge enclosed by the sphere=q = q.
The radius of the cavity is given as R2\dfrac{R}{2}.

Let the volume charge density over radius RR be ρ\rho .
q=ρ×43πR3q = \rho \times \dfrac{4}{3}\pi {R^3}
So, the charge qq' over radius R2\dfrac{R}{2} is q=ρ×43π(R2)3=ρπR36q = \rho \times \dfrac{4}{3}\pi {\left( {\dfrac{R}{2}} \right)^3} = \rho \dfrac{{\pi {R^3}}}{6}
dS=dS = enclosed area of the cavity=4π(R2)2=πR2 = 4\pi {\left( {\dfrac{R}{2}} \right)^2} = \pi {R^2}
Substituting these values in equation (1)\left( 1 \right) we get,
E.dS=qεE.dS = \dfrac{{q'}}{\varepsilon }
E=ρπR36πR2ε0 E=ρR6ε0 \Rightarrow E = \dfrac{{\rho \dfrac{{\pi {R^3}}}{6}}}{{\pi {R^2}{\varepsilon _0}}} \\\ \therefore E = \dfrac{{\rho R}}{{6{\varepsilon _0}}} \\\
Thus now we get the electric field E=ρR6ε0E = \dfrac{{\rho R}}{{6{\varepsilon _0}}}.

Note: Gauss Law is applicable in many cases as it is shown here. The electric field inside both a hollow sphere and a non-conducting sphere is 00. But the electric field inside a conducting sphere is not 00 as the charge does not reside outside the sphere.