The electric field of a plane electromagnetic wave propagating along the $x$-direction in vacuum is $\overrightarrow{E} = E_{0} \hat{j} \cos(\omega t - kx)$. The magnetic field $\overrightarrow{B}$ at the moment $t = 0$ is:

  • A
    $\overrightarrow{B} = E_{0} \sqrt{\mu_{0} \epsilon_{0}} \cos(kx) \hat{j}$
  • B
    $\overrightarrow{B} = \frac{E_{0}}{\sqrt{\mu_{0} \epsilon_{0}}} \cos(kx) \hat{k}$
  • C
    $\overrightarrow{B} = E_{0} \sqrt{\mu_{0} \epsilon_{0}} \cos(kx) \hat{k}$
  • D
    $\overrightarrow{B} = \frac{E_{0}}{\sqrt{\mu_{0} \epsilon_{0}}} \cos(kx) \hat{j}$

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