1. Transverse nature of electromagnetic waves
Electromagnetic waves are transverse waves. This means the electric field and magnetic field oscillate in directions that are perpendicular to the direction in which the wave travels.
1.1. Orientation of E, B and direction of travel
If the wave is moving along the x-axis, then usually:
- The electric field \(\vec{E}\) oscillates along the y-axis.
- The magnetic field \(\vec{B}\) oscillates along the z-axis.
- The wave itself travels along the x-axis.
So \(\vec{E}\), \(\vec{B}\), and the direction of propagation form a mutually perpendicular trio.
1.2. Compact vector representation
\(\vec{E} \perp \vec{B}, \quad \vec{E} \perp \vec{k}, \quad \vec{B} \perp \vec{k}\)
where \(\vec{k}\) is the direction of wave propagation.
2. Speed of electromagnetic waves
All electromagnetic waves travel with the same speed in vacuum, no matter what their wavelength or frequency is. This speed is a fundamental constant of nature.
2.1. Speed in vacuum
In vacuum, the speed of any electromagnetic wave is:
\(c = 3 \times 10^8 \, \text{m/s}\)
2.2. Relation with permittivity and permeability
Maxwell showed that the speed of electromagnetic waves in vacuum depends on two properties of free space: electric permittivity \(\varepsilon_0\) and magnetic permeability \(\mu_0\).
\(c = \dfrac{1}{\sqrt{\mu_0 \varepsilon_0}}\)
This was one of the biggest discoveries in physics because it linked light with electricity and magnetism.
2.3. Speed in a medium
When electromagnetic waves travel through glass, water, or any other material, they usually slow down. The new speed becomes:
\(v = \dfrac{c}{n}\)
where \(n\) is the refractive index of the medium.
3. Frequency and wavelength
Every electromagnetic wave has a frequency \(f\) and a wavelength \(\lambda\). Even though different types of EM waves look very different, they all follow the same basic relation.
3.1. Basic wave relation
The speed of a wave is related to its frequency and wavelength by:
\(v = f \, \lambda\)
For electromagnetic waves in vacuum, \(v = c\), so:
\(c = f \, \lambda\)
3.2. How wavelength and frequency are connected
If the frequency increases, the wavelength automatically decreases, because their product must always equal the speed of the wave.
For example:
- Radio waves have very large wavelengths and low frequencies.
- Gamma rays have very tiny wavelengths and extremely high frequencies.
4. Do electromagnetic waves need a medium?
A key property of electromagnetic waves is that they do not require a material medium to travel. They can move through vacuum.
4.1. Comparison with mechanical waves
Mechanical waves like sound or water waves need particles to vibrate. Without particles, they cannot propagate.
4.2. Self-sustaining field propagation
In electromagnetic waves, the disturbance is in the electric and magnetic fields themselves, not in matter. Because a changing electric field produces a changing magnetic field and vice versa, the wave keeps moving forward even in empty space.
5. Energy transport
Electromagnetic waves carry energy from one place to another. This is how sunlight reaches Earth through the vacuum of space.
5.1. Energy in fields
The energy in an electromagnetic wave is shared between the electric field and the magnetic field. In a plane wave, both fields carry equal amounts of energy.
5.2. Intensity
The intensity of an electromagnetic wave is the energy flowing per unit area per unit time.
Intensity is proportional to the square of the electric field amplitude:
\(I \propto E_0^2\)
6. Direction relation between E, B and propagation
The electric field, magnetic field, and direction of travel of an electromagnetic wave are all mutually perpendicular.
6.1. Right-hand rule idea
If you point your index finger along the direction of the electric field \(\vec{E}\), and your middle finger along the direction of the magnetic field \(\vec{B}\), then your thumb gives the direction in which the wave propagates.
6.2. Mathematical representation
\(\vec{k} = \vec{E} \times \vec{B}\)
This cross-product relation shows that the wave travels perpendicular to both fields.
7. Polarisation of electromagnetic waves
Electromagnetic waves can be polarised because they are transverse waves. Polarisation simply means restricting the direction in which the electric field oscillates.
7.1. Meaning of polarisation
If the electric field oscillates only in a single plane, the wave is said to be linearly polarised.
7.2. Everyday example
Polaroid sunglasses block certain orientations of light waves. They reduce glare because they absorb waves whose electric field oscillates in specific directions.