A series LCR circuit is connected to a variable frequency 230 V source. L = 5H, C = 80 µF & R = $40 \Omega$. The potential drop across R at resonating frequency is: |
$230 V$ $230 \sqrt{2} V$ $115 \sqrt{2} V$ 0 |
$230 V$ |
The correct answer is Option (1) → 230 V At resonance, the inductive resistance $(X_L)$ and capacitive resistance $(X_C)$ are equal: $X_L=X_C$ $⇒2πfL=\frac{1}{2πfC}$ $⇒f=\frac{1}{2π\sqrt{LC}}=\frac{1}{2π\sqrt{5×60×10^{-6}}}≃12.57Hz$ At resonance, the impedance of the circuit $Z=R$ is - $I=\frac{V_{supply}}{Z}=\frac{V_{supply}}{R}$ [By ohm's law] $=\frac{230V}{40Ω}=5.75A$ $∴V_R=I.R$ $=(5.75×40)$ $=230V$ |