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In a series resonant LCR circuit, the voltage across $R$ is 100 volts and $R=1 \mathrm{k} \Omega$ with $C=2 \mu \mathrm{F}$. The resonant frequency $\omega$ is $200 \mathrm{rad} / \mathrm{s}$. At resonance the voltage across $L$ is
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$250 \mathrm{~V}$
$250 \mathrm{~V}$
$\mathrm{i}=\frac{100}{1000}=0.1 \mathrm{~A}$
$V_L=V_C=\frac{0.1}{200 \times 2 \times 10^{-6}}=250 \mathrm{~V}$
$V_L=V_C=\frac{0.1}{200 \times 2 \times 10^{-6}}=250 \mathrm{~V}$
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