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Question: A uniform sphere of charge of radius \(a\) has electric potential at distance \(\dfrac{3a}{2}\) from...

A uniform sphere of charge of radius aa has electric potential at distance 3a2\dfrac{3a}{2} from its centre equal to half of its value at distance xx from its centre. Then, what is the value of xx?
A. Zero
B. a2\dfrac{a}{2}
C. a2\dfrac{a}{\sqrt{2}}
D. a3\dfrac{a}{\sqrt{3}}

Explanation

Solution

First, assume the charge on the sphere to be qq and find the expression of electric potential at distance 3a2\dfrac{3a}{2} and xx from its centre. Then use the given relation between electric potential at distance xx and distance 3a2\dfrac{3a}{2} from centre to obtain the magnitude of xx.
Formula used:
Electric potential due to a point charge V=kQrV=\dfrac{kQ}{r}

Complete answer:
Electric potential due to a point charge is given by
V=kQrV=\dfrac{kQ}{r}
Where k=14πϵ0k=\dfrac{1}{4\pi {{\epsilon }_{0}}} and rr is the distance of the point from the centre of the sphere.
For a uniformly charged sphere, electric field outside the sphere is equivalent to that from a point charge. This means, outside the sphere the potential is also the same as that from a point charge.

Let us assume charge on the sphere is QQ. Then electric potential at distance 3a2\dfrac{3a}{2} from centre of the sphere is
V3a/2=kQ3a/2=2kQ3a{{V}_{3a/2}}=\dfrac{kQ}{3a/2}=\dfrac{2kQ}{3a}
Electric potential at distance xx from centre is given by
Vx=kQx{{V}_{x}}=\dfrac{kQ}{x}
Since, this value of potential is equal to half of its value at distance xx from its centre. This implies that
12V3a/2=VxV3a/2=2Vx\dfrac{1}{2}{{V}_{3a/2}}={{V}_{x}}\Rightarrow {{V}_{3a/2}}=2{{V}_{x}}
Substituting the corresponding values, we have
2kQ3a=2kQx\dfrac{2kQ}{3a}=2\dfrac{kQ}{x}
We rearrange and simplify this equation and obtain,
x=a2x=\dfrac{a}{2}

So, the correct answer is “Option B”.

Note:
Read the question carefully as sometimes students may get confused about the relation between the value of electric potential at distance xx and 3a2\dfrac{3a}{2} from centre.
For a point inside the uniformly charged sphere, electric potential is
V=kQR3r2V=\dfrac{kQ}{{{R}^{3}}}{{r}^{2}}where rris the distance of point from centre and R is the radius of sphere.
Alternatively, this question can also be solved without assuming any charge on the sphere by using inverse proportionality of electric potential on distance for the same charge.
V1rV\propto \dfrac{1}{r}
From this, we have
V3a/2Vx=rxr3a/2\dfrac{{{V}_{3a/2}}}{{{V}_{x}}}=\dfrac{{{r}_{x}}}{{{r}_{3a/2}}}
Substituting rx=x{{r}_{x}}=x and r3a/2=3a2{{r}_{3a/2}}=\dfrac{3a}{2}, we get
V1V2=3a2x\dfrac{{{V}_{1}}}{{{V}_{2}}}=\dfrac{3a}{2x}
As V3a/2Vx=2\dfrac{{{V}_{3a/2}}}{{{V}_{x}}}=2, we get
x=a2x=\dfrac{a}{2}