A hemispherical bowl of mass $m$ is uniformly charged with charge density $'\sigma '$ . Electric potential due to charge distribution at a point $'A'$ is (which lies at centre of radius as shown).
A hemispherical bowl of mass $m$ is uniformly charged with charge density $'\sigma '$ . Electric potential due to charge distribution at a point $'A'$ is (which lies at centre of radius as shown).
- A
$\frac{{\sigma R}}{{4{\varepsilon _0}}}$
- B
$\frac{{\sigma R}}{{3{\varepsilon _0}}}$
- C
$\frac{{\sigma R}}{{2{\varepsilon _0}}}$
- D
$\frac{{\sigma R}}{{{\varepsilon _0}}}$
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