MHT CET · Physics · Electrostatics
A uniformly charge half ring of a radius ' \(R\) ' has linear charge density ' \(\sigma\) '. The electric potential at the centre of the half ring is \(\left(\epsilon_0=\right.\) permittivity of free space)
- A \(\frac{\sigma}{6 \epsilon_0}\)
- B \(\frac{\sigma}{2 \epsilon_0}\)
- C \(\frac{\sigma}{\epsilon_0}\)
- D \(\frac{\sigma}{4 \epsilon_0}\)
Answer & Solution
Correct Answer
(D) \(\frac{\sigma}{4 \epsilon_0}\)
Step-by-step Solution
Detailed explanation
If \(\mathrm{q}\) is charge on the ring, then the potential at the centre is given by
\(
\mathrm{V}=\frac{1}{4 \pi \varepsilon_0} \cdot \frac{\mathrm{q}}{\mathrm{R}}
\)
But \(\mathrm{q}=\sigma \times \pi \mathrm{R}\)
\(
\therefore \mathrm{V}=\frac{1}{4 \pi \varepsilon_0} \cdot \frac{\sigma \pi \mathrm{R}}{\mathrm{R}}=\frac{\sigma}{4 \varepsilon_0}
\)
\(
\mathrm{V}=\frac{1}{4 \pi \varepsilon_0} \cdot \frac{\mathrm{q}}{\mathrm{R}}
\)
But \(\mathrm{q}=\sigma \times \pi \mathrm{R}\)
\(
\therefore \mathrm{V}=\frac{1}{4 \pi \varepsilon_0} \cdot \frac{\sigma \pi \mathrm{R}}{\mathrm{R}}=\frac{\sigma}{4 \varepsilon_0}
\)
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