Q147 / 160 · AP EAMCET 2009 · Physics
Two point charges $-q$ and $+q$ are located at points $(0,0,-a)$ and $(0,0, a)$ respectively. The electric potential at a point $(0,0, z)$, where $z>a$ is
- A$\frac{q a}{4 \pi \varepsilon_0 z^2}$
- B$\frac{q}{4 \pi \varepsilon_0 a}$
- C$\frac{2 q a}{4 \pi \varepsilon_0\left(z^2-a^2\right)}$
- Correct answerD$\frac{2 q a}{4 \pi \varepsilon_0\left(z^2+a^2\right)}$
Solution
Potential at $P$ due to $(+q)$ charge
$V_1=\frac{1}{4 \pi \varepsilon_0} \cdot \frac{q}{(z-a)}$

Potential at $P$ due to $(-q)$ charge $V_2=\frac{1}{4 \pi \varepsilon_0} \cdot \frac{-q}{(z+a)}$ Total potential at $P$ due to $(A B)$ electric dipole $\begin{aligned} V & =V_1+V_2 \\ & =\frac{1}{4 \pi \varepsilon_0} \cdot \frac{q}{(z-a)}-\frac{1}{4 \pi \varepsilon_0} \frac{q}{(z+a)} \\ & =\frac{q}{4 \pi \varepsilon_0} \frac{(z+a-z+a)}{(z-a)(z+a)} \end{aligned}$ $\Rightarrow \quad V=\frac{2 q a}{4 \pi \varepsilon_0\left(z^2-a^2\right)}$

Potential at $P$ due to $(-q)$ charge $V_2=\frac{1}{4 \pi \varepsilon_0} \cdot \frac{-q}{(z+a)}$ Total potential at $P$ due to $(A B)$ electric dipole $\begin{aligned} V & =V_1+V_2 \\ & =\frac{1}{4 \pi \varepsilon_0} \cdot \frac{q}{(z-a)}-\frac{1}{4 \pi \varepsilon_0} \frac{q}{(z+a)} \\ & =\frac{q}{4 \pi \varepsilon_0} \frac{(z+a-z+a)}{(z-a)(z+a)} \end{aligned}$ $\Rightarrow \quad V=\frac{2 q a}{4 \pi \varepsilon_0\left(z^2-a^2\right)}$
Hence, the correct answer is option: 'D'.