Electromagnetic WavesMedium

Question

A magnetic field vector in an electromagnetic wave is represented by, $\overrightarrow{B} = B_{0}sin\left( 2\pi vt - \frac{2\pi x}{\lambda} \right)\widehat{j}$. Its associated electric field vector is

Options

A.$\overrightarrow{E} = - v\lambda{\text{ }B}_{0}sin\left( 2\pi vt - \frac{2\pi x}{\lambda} \right)\widehat{k}$
B.$\overrightarrow{E} = - v\lambda{\text{ }B}_{0}sin\left( 2\pi vt - \frac{2\pi x}{\lambda} \right)\widehat{i}$
C.$\overrightarrow{E} = v\lambda{\text{ }B}_{0}sin\left( 2\pi vt - \frac{2\pi x}{\lambda} \right)\widehat{k}$
D.$\overrightarrow{E} = v\lambda{\text{ }B}_{0}sin\left( 2\pi vt - \frac{2\pi x}{\lambda} \right)\widehat{i}$

Solution

Sol. [Key Concept: The field unit vectors satisfy (E-dir)$\times$(B-dir)$=$(propagation dir); with $E_{0} = v\lambda\ B_{0}$, the field E points along $- k$.]

$${\widehat{E} \times \widehat{B} = \widehat{C} }{\widehat{B} = \widehat{j} }{\widehat{C} = \widehat{i} }{\therefore\widehat{E} = - \widehat{k} }{\frac{E_{0}}{{\text{ }B}_{0}} = C = v\lambda }{E_{0} = B \times v\lambda }$$

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