If $q$ is the charge per unit area on the surface of a conductor, then the electric field intensity at a point on the surface is
  • A$\left( {\frac{q}{{{\varepsilon _0}}}} \right)$ normal to surface
  • B$\left( {\frac{q}{{2{\varepsilon _0}}}} \right)$ normal to surface
  • C$\left( {\frac{q}{{{\varepsilon _0}}}} \right)$ tangential to surface
  • D$\left( {\frac{q}{{2{\varepsilon _0}}}} \right)$ tangential to surface
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