The plane wave propagating through the dielectric has the magneti
![The plane wave propagating through the dielectric has the magneti](/img/relate-questions.png)
The plane wave propagating through the dielectric has the magnetic field component as
\(\vec H = 20{e^{ - \alpha x}}\cos \left( {\omega t - 0.25x} \right){\hat a_y}\;\frac{A}{m}\left( {{{\hat a}_x},\;{{\hat a}_y},\;\hat a} \right)z\;\) are unit vectors along x, y, and z-axis respectively). The polarization of the wave is in direction of:A. <span style=" line-height: 115%; background-image: initial; background-position: initial; background-size: initial; background-repeat: initial; background-attachment: initial; background-origin: initial; background-clip: initial;">â­<sub>x</sub></span>
B. -â<sub>z</sub>
C. <span class="math-tex">\(\frac{{\left( {{{\hat a}_x} + {{\hat a}_y}} \right)}}{{\sqrt 2 }}\)</span>
D. â<sub>y</sub>
Please scroll down to see the correct answer and solution guide.
Right Answer is: B
SOLUTION
Concept:
According to Poynting Theorem:
âE × âH = Direction of propagation
âE × ây = âx
âE = -âz
Polarization of the wave is the direction of the electric field component
Application:
Given: Magnetic field component is:
\(\vec H = 20{e^{ - az}}\cos \left( {\omega t - 0.2x} \right){\hat a_y}\;A/m\;\)
The direction of propagation of the wave is âx and the direction of the magnetic field component is ây.
∴ Polarization of the wave is -âz