24.
Read the following and answer the questions that follow.
Consider the charges $q_{1}$ and $q_{2}$ initially at infinity and determine the work done by an external agency to bring the charges to the given locations. Suppose, first the charge $q_{1}$ is brought from infinity to the point $r_{1}$. There is no external field against which work needs to be done, so work done in bringing $q_{1}$ from infinity to $r_{1}$ is zero.
From the definition of potential, work done in bringing charge $q_{2}$ from infinity to the point $r_{2}$ is $q_{2}$ times the potential at $\vec{r_{2}}$ due to $q_{1}$.
Let us calculate the potential energy of a system of three charges $q_{1}$, $q_{2}$ and $q_{3}$ located at $\vec{r_{1}}$, $\vec{r_{2}}$, $\vec{r_{3}}$ respectively as shown in the figure below. To bring $q_{1}$ first from infinity to $r_{1}$, no work is required ($W_{1}=0$).
(i) To bring $q_{2}$ from infinity to $r_{2}$. The work done in this step is
(A) $W_{2}=\frac{1}{4\pi\epsilon_{0}}\frac{2q_{1}q_{2}}{r_{12}^{3}}$
(B) $W_{2}=\frac{1}{4\pi\epsilon_{0}}\frac{q_{1}q_{2}}{r_{12}^{3}}$
(C) $W_{2}=\frac{1}{4\pi\epsilon_{0}}\frac{q_{1}q_{2}}{r_{12}^{2}}$
(D) $W_{2}=\frac{1}{4\pi\epsilon_{0}}\frac{q_{1}q_{2}}{r_{12}}$
(ii) The charges $q_{1}$ and $q_{2}$ produce a potential, which at any point P will be
(A) $V_{1,2}=\frac{1}{4\pi\epsilon_{0}}\left(\frac{q_{1}}{r_{1P}^{2}}+\frac{q_{2}}{r_{2P}^{2}}\right)$
(B) $V_{1,2}=\frac{1}{4\pi\epsilon_{0}}\left(\frac{q_{1}}{r_{1P}}+\frac{q_{2}}{r_{2P}}\right)$
(C) $V_{1,2}=\frac{1}{4\pi\epsilon_{0}}\left(\frac{q_{1}}{r_{1P}}-\frac{q_{2}}{r_{2P}}\right)$
(D) $V_{1,2}=\frac{1}{4\pi\epsilon_{0}}\left(\frac{2q_{1}}{r_{1P}}+\frac{3q_{2}}{r_{2P}}\right)$
(iii) The work done in bringing $q_{3}$ from infinity to the point $r_{3}$ is -
(A) $W_{3}=\frac{1}{4\pi\epsilon_{0}}\left(\frac{2q_{1}q_{3}}{r_{13}}+\frac{2q_{2}q_{3}}{r_{23}}\right)$
(B) $W_{3}=\frac{1}{4\pi\epsilon_{0}}\left(\frac{q_{1}q_{2}}{r_{12}}+\frac{q_{1}q_{3}}{r_{13}}\right)$
(C) $W_{3}=\frac{1}{4\pi\epsilon_{0}}\left(\frac{q_{1}q_{3}}{r_{13}}+\frac{q_{2}q_{3}}{r_{23}}\right)$
(D) $W_{3}=\frac{1}{4\pi\epsilon_{0}}\left(\frac{q_{1}q_{3}}{r_{12}}-\frac{q_{2}q_{3}}{r_{23}}\right)$
(iv) The total work done in assembling the system of three charges $q_{1}$, $q_{2}$ and $q_{3}$ at the given locations is given by
(A) $U=\frac{1}{4\pi\epsilon_{0}}\left(\frac{q_{1}q_{2}}{r_{12}}+\frac{q_{1}q_{3}}{r_{13}}+\frac{q_{2}q_{3}}{r_{23}}\right)$
(B) $U=\frac{1}{4\pi\epsilon_{0}}\left(\frac{q_{1}q_{2}}{r_{12}}-\frac{q_{1}q_{3}}{r_{13}}+\frac{q_{2}q_{3}}{r_{23}}\right)$
(C) $U=\frac{1}{4\pi\epsilon_{0}}\left(\frac{q_{1}q_{2}}{r_{12}}+\frac{q_{1}q_{3}}{r_{13}}-\frac{q_{2}q_{3}}{r_{23}}\right)$
(D) $U=\frac{1}{4\pi\epsilon_{0}}\left(\frac{q_{1}q_{2}}{r_{13}}+\frac{q_{1}q_{3}}{r_{22}}+\frac{q_{2}q_{3}}{r_{12}}\right)$