The electric field in an electromagnetic wave is given by $\overrightarrow{E} = \hat{i} 40 \cos \omega(t - \frac{z}{c}) \text{ N/C}$. The magnetic field induction of this wave is (in $SI$ units):

  • A
    $\overrightarrow{B} = \hat{i} \frac{40}{c} \cos \omega(t - \frac{z}{c}) \text{ T}$
  • B
    $\overrightarrow{B} = \hat{j} 40 \cos \omega(t - \frac{z}{c}) \text{ T}$
  • C
    $\overrightarrow{B} = \hat{k} \frac{40}{c} \cos \omega(t - \frac{z}{c}) \text{ T}$
  • D
    $\overrightarrow{B} = \hat{j} \frac{40}{c} \cos \omega(t - \frac{z}{c}) \text{ T}$

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The electric field of a plane electromagnetic wave is given by: $E_y = 69 \sin[0.6 \times 10^3 x - 1.8 \times 10^{11} t] \text{ V/m}$. The expression for the magnetic field associated with this electromagnetic wave is . . . . . . $T$.

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The magnetic field in a plane electromagnetic wave is given by
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