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Current Question (ID: 20613)
Question:
$\text{The electric field of a plane electromagnetic wave propagating, along the } x \text{ direction is vacuum is;} \quad \vec{E} = E_0 \cos(\omega t - kx) \hat{j}. \text{ The magnetic field } \vec{B} \text{ at the moment } t = 0 \text{ s is:}$
Options:
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1. $\vec{B} = \frac{E_0}{\sqrt{\mu_0 \epsilon_0}} \cos(kx) \hat{j}$
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2. $\vec{B} = E_0 \sqrt{\mu_0 \epsilon_0} \cos(kx) \hat{j}$
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3. $\vec{B} = \frac{E_0}{\sqrt{\mu_0 \epsilon_0}} \cos(kx) \hat{k}$
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4. $\vec{B} = E_0 \sqrt{\mu_0 \epsilon_0} \cos(kx) \hat{k}$
Solution:
$\text{Hint: } B_0 = \frac{E_0}{c}$ $\text{Step: Find the magnetic field } \vec{B} \text{ at the moment } t = 0 \text{ s.}$ $\text{For a plane electromagnetic wave propagating in the } x \text{ direction with an electric field is given by;} \Rightarrow \vec{E} = E_0 \cos(\omega t - kx) \hat{j},$ $\text{the magnetic field } \vec{B} \text{ is related to the electric field } \vec{E} \text{ using the following properties of electromagnetic waves:}$ $\text{The electric and magnetic fields are perpendicular to each other and to the direction of propagation.}$ $\text{The magnitude of the magnetic field is related to the electric field is given by the equation;} \Rightarrow B_0 = \frac{E_0}{c} = \frac{E_0}{\sqrt{\mu_0 \epsilon_0}} \text{ where } c \text{ is the speed of light in vacuum.}$ $\text{At } t = 0, \text{ the electric field is given by;} \Rightarrow \vec{E} = E_0 \cos(kx) \hat{j}$ $\text{For the magnetic field } \vec{B} \text{ since the wave propagates in the } x \text{ direction and the electric field is along the } y\text{-axis, the magnetic field will be along the } z\text{-axis } (\hat{k}), \text{ and its magnitude will be:}$ $\Rightarrow \vec{B} = \frac{E_0}{\sqrt{\mu_0 \epsilon_0}} \cos(kx) \hat{k}$ $\text{Hence, option (3) is the correct answer.}$
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