If a spherical charged conductor comes out from the closed surface of the sphere, then total flux emitted from the surface will be

• A

  $\frac{1}{{\mathrm{\epsilon }}_0}\times (\mathrm{the} \mathrm{charge} \mathrm{enclosed} \mathrm{by} \mathrm{surface})$

• B

  ${\mathrm{\epsilon }}_0\times (\mathrm{charge} \mathrm{enclosed} \mathrm{by} \mathrm{surface})$

• C

  $\frac{1}{4{\mathrm{\pi \epsilon }}_0}\times (\mathrm{charge} \mathrm{enclosed} \mathrm{by} \mathrm{surface})$

• D

  0