MHT CET · Physics · Electrostatics
Four point charges each \(+q\) is placed on the circumference of a circle of diameter 2 d in such a way that they form a square. The potential at the centre is proportional to
- A \(\frac{\mathrm{q}^2}{\mathrm{~d}^2}\)
- B \(\frac{q}{d}\)
- C \(\frac{d}{q}\)
- D \(\frac{\mathrm{d}^2}{\mathrm{q}^2}\)
Answer & Solution
Correct Answer
(B) \(\frac{q}{d}\)
Step-by-step Solution
Detailed explanation
As charges are placed on the circumference of circle, each charge is at a distance,
\(\mathrm{r}=\frac{\text { Diameter }}{2}=\frac{2 \mathrm{~d}}{2}=\mathrm{d}\)
\(\therefore \quad\) Potential at centre due to four point charges
\(\begin{aligned}
& =\frac{1}{4 \pi \varepsilon_0}\left[\frac{\mathrm{q}}{\mathrm{~d}}+\frac{\mathrm{q}}{\mathrm{~d}}+\frac{\mathrm{q}}{\mathrm{~d}}+\frac{\mathrm{q}}{\mathrm{~d}}\right] \\
& =\frac{1}{4 \pi \varepsilon_0} \frac{4 \mathrm{q}}{\mathrm{~d}}=4 \dot{K}\left[\frac{\mathrm{q}}{\mathrm{~d}}\right]
\end{aligned}\)
Potential \(\propto \frac{q}{d}\)
\(\mathrm{r}=\frac{\text { Diameter }}{2}=\frac{2 \mathrm{~d}}{2}=\mathrm{d}\)
\(\therefore \quad\) Potential at centre due to four point charges
\(\begin{aligned}
& =\frac{1}{4 \pi \varepsilon_0}\left[\frac{\mathrm{q}}{\mathrm{~d}}+\frac{\mathrm{q}}{\mathrm{~d}}+\frac{\mathrm{q}}{\mathrm{~d}}+\frac{\mathrm{q}}{\mathrm{~d}}\right] \\
& =\frac{1}{4 \pi \varepsilon_0} \frac{4 \mathrm{q}}{\mathrm{~d}}=4 \dot{K}\left[\frac{\mathrm{q}}{\mathrm{~d}}\right]
\end{aligned}\)
Potential \(\propto \frac{q}{d}\)
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