Power dissipated in an $LCR$ series circuit connected to an $a.c.$ source of electromotive force (emf) $\varepsilon$ is:

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

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