Three point charges $q, -2q$ and $q$ are placed along the $x$-axis at $x = -a, 0$ and $a$ respectively. As $a \rightarrow 0$ and $q \rightarrow \infty$ while $qa^2 = Q$ remains finite, the electric field at a point $P$, at a distance $x$ $(x \gg a)$ from $x = 0$ is $E = \frac{\alpha Q}{4 \pi \epsilon_0 x^\beta} \hat{i}$. Then:

  • A
    $\alpha = \beta$
  • B
    $\alpha = 2\beta$
  • C
    $\alpha = \frac{2}{3}\beta$
  • D
    $\alpha = \frac{3}{2}\beta$

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