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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$A$ plane electromagnetic wave travelling along the $X-$ direction has a wavelength of $3\, mm$. The variation in the electric field occurs in the $Y-$ direction with an amplitude of $66\, Vm^{-1}$. The equations for the electric and magnetic fields as a function of $x$ and $t$ are respectively:

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The amplitude of the magnetic field in an electromagnetic wave propagating along the $y$-axis is $6.0 \times 10^{-7} \, T$. The maximum value of the electric field in the electromagnetic wave is:

If $c$ is the speed of electromagnetic waves in vacuum,its speed in a medium of dielectric constant $K$ and relative permeability $\mu_r$ is:

For plane electromagnetic waves propagating in the positive $Z$-direction,the combination which gives the correct possible direction for $\vec{E}$ and $\vec{B}$ fields respectively is:

The direction of the Poynting vector represents:

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