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An inductance \( L \) having a resistance \( R \) is connected to an alternating source of angular frequency \( \omega \). The quality factor ' \( Q \) ' of the inductance is
(1) \( \frac{\omega L}{R} \)
(2) \( \left(\frac{\omega L}{R}\right)^{2} \)
- (3) \( \left(\frac{\mathrm{R}}{\omega \mathrm{L}}\right)^{2} \)
(4) \( \frac{R}{\omega L} \)
\( \mathrm{P} \)
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