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