The resonant frequency of a series $LCR$ circuit is $f_R$. The circuit is connected to a sinusoidally alternating e.m.f. of frequency $2 f_R$. The inductive reactance becomes $X_{L_1}$ and capacitive reactance becomes $X_{C_1}$ after changing the frequency. $X_{C_1}$ is equal to:

  • A
    $2 X_{L_1}$
  • B
    $\frac{1}{4} X_{L_1}$
  • C
    $\frac{1}{2} X_{L_1}$
  • D
    $X_{L_1}$

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