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Question

Question: The potential inside a point in a solid sphere will be: A) Same as that seen at the surface B) ...

The potential inside a point in a solid sphere will be:
A) Same as that seen at the surface
B) Will be less than what was seen at the surface
C) Will be more than what was seen at the surface
D) Will be equal to the potential at the centre

Explanation

Solution

This problem can be solved by using the direct formula for the electric potential at a point inside the sphere in terms of the distance of the point from the centre of the sphere, the total charge of the sphere and the radius of the sphere.

Formula used:
V=KQ2R3(3R2x2)V=\dfrac{KQ}{2{{R}^{3}}}\left( 3{{R}^{2}}-{{x}^{2}} \right) (xR)\left( x\le R \right)

Complete step by step answer:
We will use the direct formula for the electric potential inside a point of a solid sphere to compare the value for the electric potential for an inside point with that on the surface and at the centre.
The electric potential VV for a point inside a solid sphere of radius RR and total charge QQ is given by
V=KQ2R3(3R2x2)V=\dfrac{KQ}{2{{R}^{3}}}\left( 3{{R}^{2}}-{{x}^{2}} \right) (xR)\left( x\le R \right) --(1)
Where xx is the distance of the point from the centre of the sphere and K=9×109kg.m3s2C2K=9\times {{10}^{9}}kg.{{m}^{3}}{{s}^{-2}}{{C}^{-2}} is the universal electric constant.
For the electric potential at the centre Vcentre{{V}_{centre}}, x=0x=0.
Putting this in (1), we get
Vcentre=KQ2R3(3R202)=KQ2R3(3R20)=KQ2R3(3R2)=3KQ2R>KQ2R3(3R2x2){{V}_{centre}}=\dfrac{KQ}{2{{R}^{3}}}\left( 3{{R}^{2}}-{{0}^{2}} \right)=\dfrac{KQ}{2{{R}^{3}}}\left( 3{{R}^{2}}-0 \right)=\dfrac{KQ}{2{{R}^{3}}}\left( 3{{R}^{2}} \right)=\dfrac{3KQ}{2R}>\dfrac{KQ}{2{{R}^{3}}}\left( 3{{R}^{2}}-{{x}^{2}} \right)
Hence, the potential at the centre is greater than the potential at any other inside point.
Now, for the electric potential at the surface Vsurface{{V}_{surface}}, x=Rx=R.
Putting this in (1), we get
Vsurface=KQ2R3(3R2R2)=KQ2R3(2R2)=KQR<KQ2R3(3R2x2){{V}_{surface}}=\dfrac{KQ}{2{{R}^{3}}}\left( 3{{R}^{2}}-{{R}^{2}} \right)=\dfrac{KQ}{2{{R}^{3}}}\left( 2{{R}^{2}} \right)=\dfrac{KQ}{R} < \dfrac{KQ}{2{{R}^{3}}}\left( 3{{R}^{2}}-{{x}^{2}} \right)
Hence, the electric potential at the surface is lesser than that at any inside point.
Therefore, the correct option is C) Will be more than what was seen at the surface.

Note: The same result holds for the magnitude of gravitational potential also. This is because Coulomb’s law of electrostatic attraction’ mathematical form and Newton’s law of gravitation’s mathematical form are similar in nature and both are inverse square laws that vary inversely with the distance from the centre of a body. In fact the mathematical formula of (1) can be written for the magnitude of the gravitational potential by replacing the charge QQ with the mass MM of the body and the universal electric constant KK with the universal gravitational constant G=6.67×1011N.m2kg2G=6.67\times {{10}^{-11}}N.{{m}^{2}}k{{g}^{-2}}.