Question:

Given below are two statements: 
Statement I: Electromagnetic waves are not deflected by electric and magnetic field.
Statement II: The amplitude of electric field and the magnetic field in electromagnetic waves are related to each other as \(E_0 = \sqrt{\frac{\mu_0}{E_0}}B_0\).  
In the light of the above statements, choose the correct answer from the options given below:

Updated On: Mar 20, 2025
  • Statement I is true but statement II is false
  • Both Statement I and Statement II are false
  • Statement I is false but statement II is true
  • Both Statement I and Statement II are true
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The Correct Option is A

Solution and Explanation

- Statement I: True, as electromagnetic waves consist of oscillating electric and magnetic fields that do not experience deflection in external electric or magnetic fields.
- Statement II: False, because the relation is \(E_0 = c B_0\), not \(E_0 = \sqrt{\mu_0 / \epsilon_0} B_0\).
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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.