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Between two parallel sheets carrying equal and opposite surface charge densities, the field is

  • A.\( \rho_s/(2\epsilon_0) \)
  • B.zero
  • C.\( 2\rho_s/\epsilon_0 \)
  • D.\( \rho_s/\epsilon_0 \)

Answer: D

Each sheet contributes \( \rho_s/2\epsilon_0 \) and between them the two contributions point the same way and add. Outside the pair they point oppositely and cancel, which is why a parallel plate capacitor confines its field.

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