An inductor of inductance \(\mathrm{L}\) and resistor of resistance \(\mathrm{R}\)
are joined in series and connected by a source of frequency 0 power dissipated
in the circuit is,
(a) \(\left[\left\\{\mathrm{R}^{2}+\mathrm{c}^{2} \mathrm{~L}^{2}\right\\} /
\mathrm{V}\right]\)
(b) \(\left[\left\\{\mathrm{V}^{2} \mathrm{R}\right\\}
/\left\\{\mathrm{R}^{2}+\omega^{2} \mathrm{~L}^{2}\right\\}\right]\)
(c) \(\left[\mathrm{V} /\left\\{\mathrm{R}^{2}+\omega^{2}
\mathrm{~L}^{2}\right\\}\right]\)
(d) \(\left[\sqrt{ \left.\left\\{R^{2}+\omega^{2} L^{2}\right\\} /
V^{2}\right]}\right.\)