The charge on a parallel plate capacitor varies as $q = q_0 \cos(2\pi \nu t).$ The plates are very large and close together (area $= A,$ separation $= d$). The displacement current through the capacitor is

  • A
    $q_0 \, 2\pi \nu \sin(2\pi \nu t)$
  • B
    $-q_0 \, 2\pi \nu \sin(2\pi \nu t)$
  • C
    $q_0 \, 2\pi \sin(\pi \nu t)$
  • D
    $q_0 \, \pi \nu \sin(2\pi \nu t)$

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