Three charges, each equal to +q, are placed at the corners of an equilateral triangle ABC of side 'a' as shown in the figure. P and R are the mid-points of BC and CA. The work done in taking a charge Q from point P to R is: |
$\frac{3qQ}{4πε_0a}$ $\frac{3qQ}{12πε_0a}$ $\frac{qQ}{4πε_0a}$ Zero |
Zero |
The correct answer is Option (4) → Zero Work done in moving a charge $Q$ from point $P$ to $R$ in an electrostatic field is: $W = Q \, \big(V_R - V_P\big)$ Potentials at $P$ and $R$ are due to the three charges $+q$ at vertices $A, B, C$ of an equilateral triangle of side $a$. Coordinates approach:
Potential at $P$: Distances: $PB = PC = a/2$, $PA = \sqrt{3}a/2$. $V_P = kq \Big(\frac{1}{a/2} + \frac{1}{a/2} + \frac{1}{\sqrt{3}a/2}\Big)$ $V_P = kq \Big(\frac{2}{a/2} + \frac{1}{(\sqrt{3}/2)a}\Big)$ $V_P = kq \Big(\frac{4}{a} + \frac{2}{\sqrt{3}a}\Big)$ Potential at $R$: Distances: $RA = RC = a/2$, $RB = \sqrt{(3a/4)^2 + (\sqrt{3}a/4)^2} = \sqrt{12a^2/16} = \frac{\sqrt{3}a}{2}$. $V_R = kq \Big(\frac{1}{a/2} + \frac{1}{a/2} + \frac{1}{\sqrt{3}a/2}\Big)$ $V_R = kq \Big(\frac{2}{a/2} + \frac{1}{(\sqrt{3}/2)a}\Big)$ $V_R = kq \Big(\frac{4}{a} + \frac{2}{\sqrt{3}a}\Big)$ Comparison: $V_R = V_P$ Thus, $W = Q (V_R - V_P) = 0$ Answer: Work done = 0 |