Power dissipated in an $LCR$ series circuit connected to an $A.C.$ source of $e.m.f.$ $\varepsilon$ is

  • A
    $\frac{\varepsilon^2 \sqrt{R^2 + (\omega L - \frac{1}{\omega C})^2}}{R}$
  • B
    $\frac{\varepsilon^2 R^2 + (\omega L - \frac{1}{\omega C})^2}{R}$
  • C
    $\frac{\varepsilon^2 R}{\sqrt{R^2 + (\omega L - \frac{1}{\omega C})^2}}$
  • D
    $\frac{\varepsilon^2 R}{R^2 + (\omega L - \frac{1}{\omega C})^2}$

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