Power delivered by the source of the circuit becomes maximum,when

  • A
    $\omega L = \omega C$
  • B
    $\omega L = \frac{1}{\omega C}$
  • C
    $\omega L = - \left( \frac{1}{\omega C} \right)^2$
  • D
    $\omega L = \sqrt{\omega C}$

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At resonance,the value of current in a series $L-C-R$ circuit is: (Symbols have their usual meanings.)

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Two circuits are shown in the figures $(a)$ and $(b)$. At a frequency of $....\,rad/s$,the average power dissipated in one cycle will be the same in both circuits.

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