
In electromagnetic waves the ratio of amplitude of electric field and magnetic field is equal to
Answer
478.2k+ views
Hint: Consider an EM wave propagating in the z-direction. Write an equation for electric and magnetic fields in terms of the direction of propagation and time.Then use Ampere-Maxwell law for EM waves to determine the ratio of the amplitude of electric field and magnetic field in EM wave.
Formula Used:
Let us consider a plane electromagnetic wave traveling along the z-direction. Therefore, the electric and magnetic fields are functions of z-coordinate at a given time t. Electric and magnetic fields in electromagnetic waves are always perpendicular to each other as well as to the direction of propagation of the EM wave.
The electric field $E$ is along the x-axis and varies sinusoidally with z, at a given time. The magnetic field $B$is along the y axis and it also varies sinusoidally with z. We can write $E$ and $B$ as follows:
\[E{\text{ = }}{E_0}{\text{ }}sin\left( {kz - \omega t} \right)\]
\[\Rightarrow {\text{B = }}{{\text{B}}_0}{\text{ }}sin\left( {kz - \omega t} \right)\]
Here K is the magnitude of the propagation vector, $\overrightarrow K $ and its direction gives the direction of propagation of the waves K is given by
$k = \dfrac{{2\pi }}{\lambda }$
$\omega $ is the angular frequency of the wave
Now,
$\dfrac{{\partial E}}{{\partial t}} = \omega {E_0}\cos (kz - \omega t)$
$\Rightarrow \nabla \times \overrightarrow B = k{B_0}\cos (kz - \omega t)$
Using Ampere-Maxwell’s law for electromagnetic waves
$\nabla \times \overrightarrow B $=$\dfrac{1}{{{c^2}}}\dfrac{{\partial E}}{{\partial t}}$
We get
$k{B_0}\cos (kz - \omega t)$$ = {\mu _0}\overrightarrow J + \dfrac{1}{{{C^2}}}\omega {E_0}\cos (kz - \omega t)\widehat i$
$\Rightarrow k{B_0} = \dfrac{{\omega {E_0}}}{{{c^2}}}$
$\Rightarrow \dfrac{{{c^2}k}}{\omega } = \dfrac{{{E_0}}}{{{B_0}}}$
The velocity of a wave is given by $\nu = \dfrac{\omega }{k}$ and we know that the velocity of EM waves is equal to the velocity of light. Therefore
$\dfrac{\omega }{k} = c$
Substituting this value in the previous equation we get,
$\therefore \dfrac{{{E_0}}}{{{B_0}}} = c$
Hence, we conclude that the ratio of electric field and magnetic field in the EM wave is equal to the speed of light in free space.
Note: In an EM wave, the magnetic energy density is equal to the electrical energy density. EM waves do not require any medium to propagate which makes them different from other waves. The magnitude of the velocity of propagation of an EM wave is equal to that of the speed of light.
Formula Used:
Let us consider a plane electromagnetic wave traveling along the z-direction. Therefore, the electric and magnetic fields are functions of z-coordinate at a given time t. Electric and magnetic fields in electromagnetic waves are always perpendicular to each other as well as to the direction of propagation of the EM wave.
The electric field $E$ is along the x-axis and varies sinusoidally with z, at a given time. The magnetic field $B$is along the y axis and it also varies sinusoidally with z. We can write $E$ and $B$ as follows:
\[E{\text{ = }}{E_0}{\text{ }}sin\left( {kz - \omega t} \right)\]
\[\Rightarrow {\text{B = }}{{\text{B}}_0}{\text{ }}sin\left( {kz - \omega t} \right)\]
Here K is the magnitude of the propagation vector, $\overrightarrow K $ and its direction gives the direction of propagation of the waves K is given by
$k = \dfrac{{2\pi }}{\lambda }$
$\omega $ is the angular frequency of the wave
Now,
$\dfrac{{\partial E}}{{\partial t}} = \omega {E_0}\cos (kz - \omega t)$
$\Rightarrow \nabla \times \overrightarrow B = k{B_0}\cos (kz - \omega t)$
Using Ampere-Maxwell’s law for electromagnetic waves
$\nabla \times \overrightarrow B $=$\dfrac{1}{{{c^2}}}\dfrac{{\partial E}}{{\partial t}}$
We get
$k{B_0}\cos (kz - \omega t)$$ = {\mu _0}\overrightarrow J + \dfrac{1}{{{C^2}}}\omega {E_0}\cos (kz - \omega t)\widehat i$
$\Rightarrow k{B_0} = \dfrac{{\omega {E_0}}}{{{c^2}}}$
$\Rightarrow \dfrac{{{c^2}k}}{\omega } = \dfrac{{{E_0}}}{{{B_0}}}$
The velocity of a wave is given by $\nu = \dfrac{\omega }{k}$ and we know that the velocity of EM waves is equal to the velocity of light. Therefore
$\dfrac{\omega }{k} = c$
Substituting this value in the previous equation we get,
$\therefore \dfrac{{{E_0}}}{{{B_0}}} = c$
Hence, we conclude that the ratio of electric field and magnetic field in the EM wave is equal to the speed of light in free space.
Note: In an EM wave, the magnetic energy density is equal to the electrical energy density. EM waves do not require any medium to propagate which makes them different from other waves. The magnitude of the velocity of propagation of an EM wave is equal to that of the speed of light.
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