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Question: The surface density of charge on a sphere of a radius \(R\) in terms of electric intensity \(E\) at ...

The surface density of charge on a sphere of a radius RR in terms of electric intensity EE at a distance rr in free space is:
(A). ε0E(Rr)2{\varepsilon _0}E{\left( {\dfrac{R}{r}} \right)^2}
(B). ε0ERr2\dfrac{{{\varepsilon _0}ER}}{{{r^2}}}
(C). ε0E(rR)2{\varepsilon _0}E{\left( {\dfrac{r}{R}} \right)^2}
(D). ε0ErR2\dfrac{{{\varepsilon _0}Er}}{{{R^2}}}

Explanation

Solution

In this problem, we have to calculate the surface charge density ( σ\sigma ) of the sphere by using the equation σ=QA\sigma = \dfrac{Q}{A} . So, first calculate the value of QQ using the equation for the electric field, i.e. E=Q4πε0r2E = \dfrac{Q}{{4\pi {\varepsilon _0}{r^2}}} . Then calculate the value of AA using the equation for the surface area of a sphere, i.e. A=4πR2A = 4\pi {R^2} . Then put these values in the equation σ=QA\sigma = \dfrac{Q}{A} to reach the solution.

Complete step-by-step answer :
In this problem, we are given a charged sphere that has a radius RR and the electric field intensity at a distance rr is EE and we have to calculate the surface charge density (the amount of charge distributed per unit surface area).
Let the surface charge density of the sphere be σ\sigma , the total charge on the sphere be QQ and the surface area of the sphere be AA .
So, σ=QA\sigma = \dfrac{Q}{A}
After seeing the above equation it becomes clear that to calculate the value of surface charge density ( σ\sigma ) we have to first calculate the total charge on the sphere ( QQ ) and the surface area of the entire sphere ( AA ).
We know that the electric field EE due to a charger sphere having a total charge QQ at any distance rr is given by the equation
E=Q4πε0r2E = \dfrac{Q}{{4\pi {\varepsilon _0}{r^2}}}
This equation is calculated assuming that the total charge in the sphere will behave as a point charge.
Q=4πε0r2EQ = 4\pi {\varepsilon _0}{r^2}E
We also know that the surface area of the sphere of a radius RR is given by the equation
A=4πR2A = 4\pi {R^2}
So, the surface charge density σ\sigma is
σ=QA\sigma = \dfrac{Q}{A}
σ=4πε0r2E4πR2\sigma = \dfrac{{4\pi {\varepsilon _0}{r^2}E}}{{4\pi {R^2}}}
σ=ε0Er2R2\sigma = \dfrac{{{\varepsilon _0}E{r^2}}}{{{R^2}}}
σ=ε0E(rR)2\sigma = {\varepsilon _0}E{\left( {\dfrac{r}{R}} \right)^2}
Hence, option C is the correct choice.

Note : In the solution above, during the process of calculating the electric field due to the charged sphere at a distance rr , we assumed the sphere to be a point charge. This was done to simplify the solution because, in reality, all the charges spread on the surface of the sphere have different distances from the point for which we have to calculate the electric field.