An inductor of inductance $L$ and resistor $R$ are joined together in series and connected to a source of frequency $\omega$. The power dissipated in the circuit is

  • A
    $\frac{V^2}{R^2+\omega^2 L^2}$
  • B
    $\frac{R^2+\omega^2 L^2}{V^2}$
  • C
    $\frac{V^2 R}{\sqrt{R^2+\omega^2 L^2}}$
  • D
    $\frac{V^2 R}{R^2+\omega^2 L^2}$

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