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Question

Question: How does Gauss law work inside a conducting sphere?...

How does Gauss law work inside a conducting sphere?

Explanation

Solution

An electric conductor has a very large number of charges that moves freely inside the sphere. In the conducting sphere, at all the points inside the sphere, the electric field is zero.

Complete step by step answer:
Let us consider a uniformly charged sphere. The uniformly charged sphere has a radius of RR. It has a total charge QQ. The electric field inside the sphere can be found using the Gauss law.
Have the diagram for reference. Consider the point PP that is inside the shell that is placed at the distance rr from the center.

In the diagram, for the points inside the spherical sphere, a spherical gaussian surface is drawn smaller than the spherical sphere
The gaussian surface is drawn around the sphere with the radius. Now let us apply the gauss law. If a charge QQ is enclosed an arbitrary closed surface, then the total electric flux through the closed surface is,
ϕE=E.dA\Rightarrow {\phi _E} = \oint {\overrightarrow E .d\overrightarrow A }
Applying the gauss law,
E.dA=Qε0\Rightarrow \oint {\overrightarrow E .d\overrightarrow A = \dfrac{Q}{{{\varepsilon _0}}}}
Substitute the value of the area in the formula we get,
E.4πr2=Qε0\Rightarrow E.4\pi {r^2} = \dfrac{Q}{{{\varepsilon _0}}}
Gaussian surface encloses no charge, that is Q=0Q = 0 . Substitute the charge value in the equation,
E.4πr2=0ε0\Rightarrow E.4\pi {r^2} = \dfrac{0}{{{\varepsilon _0}}}
Zero divided by any number is zero. The value of the electric field will become zero. That is,
E=0\Rightarrow E = 0
From this, we are able to understand that the electric field due to the uniformly charged sphere is zero at all the points inside the shell.

Note:
Suppose if the electric field inside the sphere is not zero then there will be a force acting on the mobile carriers due to the electric field. Due to this, there will be a net motion of the mobile charge carriers that contradicts the conductor being in the electrostatic equilibrium.