If an electromagnetic wave propagating through vacuum is described by $E_y = E_0 \sin(kx - \omega t)$ and $B_z = B_0 \sin(kx - \omega t)$,then:

  • A
    $E_0 k = B_0 \omega$
  • B
    $E_0 B_0 = \omega k$
  • C
    $E_0 \omega = B_0 k$
  • D
    $E_0 B_0 = \frac{\omega}{k}$

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