Correct answer is (c) \(\frac {(q \, log2)}{a}\)
Best explanation: The total potential energy at the origin due to the system is V=\(\frac {q}{a} – \frac {q}{2a} + \frac {q}{3a} – \frac {q}{4a} + \frac {q}{5a}\)……(up to infinity), where a, 2a, 3a… are the distances of the charges from the origin. Now, taking \(\frac {q}{a}\) common from the terms, we get V=\(\frac {q}{a} (1 – \frac {1}{2} + \frac {1}{3} – \frac {1}{4} + \frac {1}{5})\). By substituting the expansion of log2, we can get V=\(\frac {(q \, log2)}{a}\).