If the uniform surface charge density on the infinite plane sheet is $\mathrm{\sigma }$, electric field near the surface will be :

• A

  $\frac{\mathrm{\sigma }}{2{\mathrm{\epsilon }}_0}$

• B

  $\frac{3\mathrm{\sigma }}{{\mathrm{\epsilon }}_0}$

• C

  $\frac{\mathrm{\sigma }}{{\mathrm{\epsilon }}_0}$

• D

  $\frac{2\mathrm{\sigma }}{{\mathrm{\epsilon }}_0}$