The electric field in an electromagnetic wave is given by \[ \vec{E} = \hat{i} 40 \cos \omega \left( t - \frac{z}{c} \right) \, \text{NC}^{-1}.\]The magnetic field induction of this wave is (in SI unit):
Given the electric field of the electromagnetic wave: \[ \vec{E} = \hat{i} 40 \cos \omega \left( t - \frac{z}{c} \right) \, \text{NC}^{-1} \] In an electromagnetic wave, the magnetic field \(\vec{B}\) is perpendicular to both the electric field \(\vec{E}\) and the direction of propagation.
Since \(\vec{E}\) is along the \(\hat{i}\)-direction and the wave propagates along the \(\hat{k}\)-direction, the magnetic field \(\vec{B}\) must be along the \(\hat{j}\)-direction.
The relationship between the magnitudes of the electric and magnetic fields in an electromagnetic wave is given by: \[ B = \frac{E}{c} \]
Substituting the given electric field magnitude: \[ B = \frac{40}{c} \cos \omega \left( t - \frac{z}{c} \right) \] Thus, the magnetic field is: \[ \vec{B} = \hat{j} \frac{40}{c} \cos \omega \left( t - \frac{z}{c} \right) \]
