This tutorial explores wave propagation. Whether used in radio frequency systems, microwave systems, optical system or other, electromagnetic waves propagation obey Maxwell's equations. Here we try to examine one of the simplest solution to Maxwell's equation and understand its meaning. An electromagnetic field with only one component Ex and independent of x and y is solution to the differential equation
The above equation has many solutions. However one of the simplest and most useful is the one where time and z variations are sinusoidal and is given by.
The electric field component Ex is a function of two variables: t and z. To study this function we will change time t in steps and plot Ex as a function of z. This is done in the applet below.
Explore wave propagation using the equation: \[ E_x = E_0 \cos(\omega t - kz) \]
The red curve shows the electric field Eₓ as it varies with position z at the current time t.
Time Evolution (Period T): At a fixed position (choose any vertical line), watch how the wave oscillates up and down. The time between successive peaks at that position is the period T.
Spatial Variation (Wavelength λ): At a fixed time (pause the animation), measure the distance between two successive peaks. This distance is the wavelength λ.
Wave Propagation: The wave moves to the right because of the minus sign in \[ \omega t - kz \]. This means that as time increases, the wave pattern shifts to the right.
Key Relationships:
Try adjusting the frequency and wavelength sliders independently to see how they affect the wave's appearance and speed.
More on antennas antennas and parabolic reflectors.