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In A.C. voltage source, v = v0 sin t; having a fixed value for v0 , but of variable frequency, is connected across a given series LCR circuit. The variation of the current I, flowing in the circuit, with ω, (the angular frequency ofthe source) is as shown. The power consumption, in the circuit, at (angular) frequencies ω1 and ω2 , is

(1) 50% of that at (angular)frequency ω0 and the difference, (ω2- ω1), increases with an increase in the Q-factor of the circuit

(2) 50% of that at (angular) frequency ω0 and the difference, (ω2- ω1), decreases with an increase in the Q-factor of the circuit

(3) (nearly) 71% of that at (angular) frequency ω0 and the difference, (ω2- ω1) , decreases with an increase in the ‘Q-factor’ of the circuit

(4) (nearly) 71% of that at (angular) frequency ω0 and the difference, (ω2- ω1) , increases with an increase in the ‘Q-factor’ of the circuit

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(2) 50% of that at (angular) frequency ω0 and the difference, (ω2- ω1), decreases with an increase in the Q-factor of the circuit

The current value, for ω1 and ω2 , is 1/√2 times the current value at ω0 . Hence the power consumption (αI2) would become (1/2) or 50% of that at ω0 .

Further, the more the value of Q, the sharper is the resonance of the circuit. This implies that there is a decrease, in the difference, (ω- ω1) when the Q-further increases.

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