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The charge on a parallel plate capacitor varies as
\( \mathrm{P} \) \( q=q_{0} \cos 2 \pi v t \). The plates are very large and

W close together \( ( \) area \( =A \), separation \( =d) \). The displacement current through the capacitor is
(1) \( q_{0} 2 \pi u \sin \pi u t \)
(2) \( -q_{0} 2 \pi u \sin 2 \pi u t \)
(3) \( q_{0} 2 \pi \sin \pi u t \)
(4) \( q_{0} \pi u \sin 2 \pi u t \)
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