The electric field component of a monochromatic radiation is given by
$\vec E = 2E_0 \hat i \cos kz \cos \omega t$
Its magnetic field $\vec B$ is then given by

  • A
    $\frac{2E_0}{c} \hat j \sin kz \cos \omega t$
  • B
    $-\frac{2E_0}{c} \hat j \sin kz \sin \omega t$
  • C
    $\frac{2E_0}{c} \hat j \sin kz \sin \omega t$
  • D
    $\frac{2E_0}{c} \hat j \cos kz \cos \omega t$

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