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Question: Calculate the electric potential at the center of the square in figure ![](https://www.vedantu....

Calculate the electric potential at the center of the square in figure

Explanation

Solution

Hint To find the potential at the center, we need to calculate the potential at the center due to each of the charges. And the distance of the charges from the center will be half of the diagonal of the square given.

Formula Used:
In this solution we will be using the following formula,
V=kqr\Rightarrow V = \dfrac{{kq}}{r}
where VV is the potential, qq is the charge and rr is the distance.

Complete step by step answer
In the given diagram in the question we can see that the charges are placed in the form of a square and we need to find the potential at the center of this square.
Now the distance of each charge will be half of the diagonal of the square of side 0.10m0.10m .
Now we have the value of the diagonal as, d=0.12+0.12d = \sqrt {{{0.1}^2} + {{0.1}^2}}
So calculating we have,
d=2×0.1\Rightarrow d = \sqrt {2 \times 0.1}
Now the distance of the charge from the center is given as,
r=d2\Rightarrow r = \dfrac{d}{2}
So we get, r=2×0.122=0.122r = \dfrac{{\sqrt {2 \times {{0.1}^2}} }}{2} = 0.1\dfrac{{\sqrt 2 }}{2}
Hence the distance is, r=0.12r = \dfrac{{0.1}}{{\sqrt 2 }}
Therefore each of the charges is at a distance r=0.12r = \dfrac{{0.1}}{{\sqrt 2 }} .
Now the potential is given as, V=kqrV = \dfrac{{kq}}{r}
The potential at the center will be the sum of the potential due to each of the charges,
V=kq1r+kq2r+kq3r+kq4r\Rightarrow V = \dfrac{{k{q_1}}}{r} + \dfrac{{k{q_2}}}{r} + \dfrac{{k{q_3}}}{r} + \dfrac{{k{q_4}}}{r}
Taking common kr\dfrac{k}{r} we get,
V=kr[q1+q2+q3+q4]\Rightarrow V = \dfrac{k}{r}\left[ {{q_1} + {q_2} + {q_3} + {q_4}} \right]
In the question we are given, q1=10μC{q_1} = - 10\mu C , q2=10μC{q_2} = - 10\mu C , q3=5.0μC{q_3} = 5.0\mu C and q4=5.0μC{q_4} = 5.0\mu C
Now substituting we get,
V=kr[1010+5+5]×106\Rightarrow V = \dfrac{k}{r}\left[ { - 10 - 10 + 5 + 5} \right] \times {10^{ - 6}}
On calculating we get, V=kr[10]×106V = \dfrac{k}{r}\left[ { - 10} \right] \times {10^{ - 6}}
The value of kk is 9×1099 \times {10^9} so substituting we get,
V=9×1090.12×10×106\Rightarrow V = - \dfrac{{9 \times {{10}^9}}}{{\dfrac{{0.1}}{{\sqrt 2 }}}} \times 10 \times {10^{ - 6}}
So we get,
V=9×1090.1×102×106\Rightarrow V = - \dfrac{{9 \times {{10}^9}}}{{0.1}} \times 10\sqrt 2 \times {10^{ - 6}}
On calculating we have,
V=92×105\Rightarrow V = - 9\sqrt 2 \times {10^5}
So we get the potential at the center as,
V=1.27×106V\Rightarrow V = - 1.27 \times {10^6}V .

Note
The electric potential at a point is the amount of work which is needed to move a charge from a reference point to the given point in an electric field without producing acceleration. Typically we take the reference point at infinity.