\(-\hat{j}+\hat{k},-\hat{j}+\hat{k}\)
\(\hat{j}+\hat{k},\hat{j}+\hat{k}\)
\(-\hat{j}+\hat{k},-\hat{j}-\hat{k}\)
\(\hat{j}+\hat{k},-\hat{j}-\hat{k}\)
To solve this problem, we need to understand the properties of electromagnetic waves (EM waves). In a plane electromagnetic wave, the electric field (\( \mathbf{E} \)) and the magnetic field (\( \mathbf{B} \)) are perpendicular to each other and both are perpendicular to the direction of propagation of the wave.
For a plane electromagnetic wave propagating in the \(x\)-direction, the direction of these fields can be determined by the following rules:
Let's consider each option to see which fits these criteria:
Therefore, the correct choice is option three, \(-\hat{j}+\hat{k},-\hat{j}-\hat{k}\), where the electric field and magnetic field are correctly oriented such that their cross product results in the propagation along the \(x\)-direction.
The dimension of $ \sqrt{\frac{\mu_0}{\epsilon_0}} $ is equal to that of: (Where $ \mu_0 $ is the vacuum permeability and $ \epsilon_0 $ is the vacuum permittivity)
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.
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: