Question:

In a plane electromagnetic wave, the electric field oscillates sinusoidally at a frequency of \(2.0 × 10^10 \ Hz\) and amplitude \(48\  V m^{−1}\)

  1. What is the wavelength of the wave?
  2. What is the amplitude of the oscillating magnetic field?
  3. Show that the average energy density of the E field equals the average energy density of the B field. \([c = 3 × 10^8 m s^{−1}]\)

Updated On: Sep 29, 2023
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Solution and Explanation

Frequency of the electromagnetic wave, \(ν = 2.0 × 10^{10} Hz\)
Electric field amplitude, \(E_0 = 48\  V m^{−1 }\)
Speed of light, \(c = 3 × 10^8 \ m/s\) 


\((a)\) Wavelength of a wave is given as:

\(λ = \frac {c}{v}\)

\(λ =\frac { 3\times 10^8}{2\times 10^{10}}\)

\(λ = 0.015\  m\)


\((b)\) Magnetic field strength is given as: 

\(B_o =\frac { E_o}{c}\)

\(B_o = \frac{48}{3\times 10^8}\)

\(B_0 = 1.6\times 10^{-7} T\)


\((c)\)Energy density of the electric field is given as:

\(U_E = \frac {1}{2} ε_oE^2\)

And, energy density of the magnetic field is given as:

\(U_B = \frac {1}{2 µ_0} B^2\)

Where, 
\(ε_0\) = Permittivity of free space 
\(µ_0\) = Permeability of free space 
We have the relation connecting E and B as: 
E = cB     .… (1) 
Where,

\(c = \frac {1}{\sqrt {ε_0µ_0}}\)    .....(2)

Putting equation (2) in equation (1), we get

\(E = \frac {1}{\sqrt {ε_0µ_0}} B\)

Squaring both sides, we get

\(E^2 = \frac {1}{ {ε_0µ_0}} B^2\)

\(ε_0E^2 = \frac {B^2}{µ_0}\)

\(\frac 12 ε_0E^2 = \frac 12 \frac {B^2}{µ_0}\)

\(⇒ U_E = U_B\)

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Notes on Electromagnetic Waves

Concepts Used:

Electromagnetic waves

The waves that are produced when an electric field comes into contact with a magnetic field are known as Electromagnetic Waves or EM waves. The constitution of an oscillating magnetic field and electric fields gives rise to electromagnetic waves.

Types of Electromagnetic Waves:

Electromagnetic waves can be grouped according to the direction of disturbance in them and according to the range of their frequency. Recall that a wave transfers energy from one point to another point in space. That means there are two things going on: the disturbance that defines a wave, and the propagation of wave. In this context the waves are grouped into the following two categories:

  • Longitudinal waves: A wave is called a longitudinal wave when the disturbances in the wave are parallel to the direction of propagation of the wave. For example, sound waves are longitudinal waves because the change of pressure occurs parallel to the direction of wave propagation.
  • Transverse waves: A wave is called a transverse wave when the disturbances in the wave are perpendicular (at right angles) to the direction of propagation of the wave.