Step 1: Definition of Electromagnetic Waves:
Electromagnetic (EM) waves are disturbances consisting of time-varying, sinusoidal electric and magnetic fields that oscillate perpendicular to each other and also perpendicular to the direction of wave propagation.
Key properties include:
They are transverse in nature.
They are produced by accelerating electric charges.
They do not require a material medium for their propagation and can travel through a vacuum.
In a vacuum, they travel at a constant speed, the speed of light, \( c \approx 3 \times 10^8 \) m/s.
The electric field (\(\vec{E}\)) and magnetic field (\(\vec{B}\)) are always in the same phase.
Step 2: Propagation Diagram:
The diagram below shows the orientation of the electric field, magnetic field, and the direction of propagation for a plane-polarized electromagnetic wave.
\begin{center}
\begin{tikzpicture}[scale=1.5, transform shape]
% Axes
\draw[→, thick] (0,0,0) -- (4,0,0) node[below] {X (Propagation)};
\draw[→, thick] (0,0,0) -- (0,1.5,0) node[left] {Y (E-field)};
\draw[→, thick] (0,0,0) -- (0,0,1.5) node[below right] {Z (B-field)};
% E-field wave (in XY plane)
\draw[red, thick] plot[domain=0:3.5, samples=100] (\x, {sin(\x*180/pi r)}, 0);
% Arrows for E-field
\foreach \x in {0.5, 2.5} {
\draw[→, red, thick] (\x*pi/2, 0, 0) -- (\x*pi/2, {sin(\x*pi/2*180/pi r)}, 0) node[left] {\(\vec{E}\)};
}
% B-field wave (in XZ plane)
\draw[blue, thick] plot[domain=0:3.5, samples=100] (\x, 0, {sin(\x*180/pi r)});
% Arrows for B-field
\foreach \x in {0.5, 2.5} {
\draw[→, blue, thick] (\x*pi/2, 0, 0) -- (\x*pi/2, 0, {sin(\x*pi/2*180/pi r)}) node[below right] {\(\vec{B}\)};
}
\end{tikzpicture}
\end{center}
Diagram Explanation:
The wave is propagating along the positive X-axis.
The electric field vector \(\vec{E}\) (in red) oscillates along the Y-axis.
The magnetic field vector \(\vec{B}\) (in blue) oscillates along the Z-axis.
At every point and every instant, \(\vec{E}\) is perpendicular to \(\vec{B}\), and both are perpendicular to the direction of propagation.
The vectors \(\vec{E}\), \(\vec{B}\), and the propagation vector \(\vec{k}\) form a right-handed system (\(\vec{E} \times \vec{B}\) points in the direction of propagation).