An inductor of inductance L and resistor of resistance R are joined in series and connected by a source of frequency ω power dissipated in the circuit is,
Options:
(a) `((R^2+omega^2+L^2))/V `
(b) `(V^2R)/((R^2+omega^2+L^2))`
(c) `V/((R^2+omega^2+L^2))`
(d) `sqrt(R^2+omega^2+L^2)/V^2`