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

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

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