Let $\sigma$ be the uniform surface charge density of two infinite thin plane sheets shown in the figure. Then the electric fields in three different regions $I, II$ and $III$ are:

  • A
    $\vec{E}_{ I }=\frac{2 \sigma}{\epsilon_0} \hat{n}, \vec{E}_{ II }=0, \vec{E}_{ III }=\frac{2 \sigma}{\epsilon_0} \hat{n}$
  • B
    $\vec{E}_{ I }=0, \vec{E}_{ II }=\frac{\sigma}{\epsilon_0} \hat{n}, \vec{E}_{ III }=0$
  • C
    $\vec{E}_{ I }=\frac{\sigma}{2 \epsilon_0} \hat{n}, \vec{E}_{ II }=0, \vec{E}_{ III }=\frac{\sigma}{2 \epsilon_0} \hat{n}$
  • D
    $\vec{E}_{ I }=-\frac{\sigma}{\epsilon_0} \hat{n}, \vec{E}_{ II }=0, \vec{E}_{ III }=\frac{\sigma}{\epsilon_0} \hat{n}$

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