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Physics · Ch 8 — Electromagnetic Waves

Nature of Electromagnetic Waves

8.3.2

Nature of Electromagnetic Waves

Nature of Electromagnetic Waves

Electromagnetic waves are self-sustaining oscillations of electric and magnetic fields. From Maxwell’s equations, a key result emerges: in an electromagnetic wave, the electric field E\mathbf{E} and the magnetic field B\mathbf{B} are perpendicular to each other, and both are perpendicular to the direction of wave propagation. This is a general feature.

Why are E\mathbf{E} and B\mathbf{B} perpendicular?

Consider a charging capacitor (Fig. 8.2). The electric field inside the plates is perpendicular to the plates. The displacement current produces a magnetic field that circles around the plates (parallel to them). Thus, E\mathbf{E} and B\mathbf{B} are perpendicular in this case. This property holds for all electromagnetic waves.

Mathematical Description of a Plane Wave

A typical plane electromagnetic wave propagating along the zz-direction is shown in Fig. 8.3. At a given time tt, the electric field oscillates along the xx-axis, and the magnetic field oscillates along the yy-axis. Both vary sinusoidally with zz.

The electric field ExE_x and magnetic field ByB_y are given by:

Ex=E0sin⁡(kz−ωt)E_x = E_0 \sin(kz - \omega t)

By=B0sin⁡(kz−ωt)B_y = B_0 \sin(kz - \omega t)

Here:

  • E0E_0 and B0B_0 are the amplitudes of the electric and magnetic fields.
  • kk is the magnitude of the wave vector (or propagation vector) k\mathbf{k}. Its direction gives the direction of propagation.
  • ω\omega is the angular frequency.
  • The wave propagates with speed v=ω/kv = \omega/k.
Relation Between kk and λ\lambda

The wave number kk is related to the wavelength λ\lambda by:

k=2πλk = \frac{2\pi}{\lambda}

Speed of Electromagnetic Waves in Vacuum

Using Maxwell’s equations with the wave equations for ExE_x and ByB_y, we find that ω=ck\omega = ck, where cc is the speed of light in vacuum:

c=1μ0ε0c = \frac{1}{\sqrt{\mu_0 \varepsilon_0}}

This is a fundamental constant. In terms of frequency ν=ω/2π\nu = \omega/2\pi and wavelength λ=2π/k\lambda = 2\pi/k, the relation becomes:

νλ=c\nu \lambda = c

Relation Between Electric and Magnetic Field Amplitudes

From Maxwell’s equations, the magnitudes of the electric and magnetic fields in an electromagnetic wave are related by:

B0=E0cB_0 = \frac{E_0}{c}

This means that at any instant, the ratio of the electric field magnitude to the magnetic field magnitude is cc.

Electromagnetic Waves in a Material Medium

In a material medium with permittivity ε\varepsilon and magnetic permeability μ\mu, the speed of light becomes:

v=1μεv = \frac{1}{\sqrt{\mu \varepsilon}}

Thus, the speed of light depends on the electric and magnetic properties of the medium. The refractive index of one medium relative to another is the ratio of the speeds of light in the two media. …

Figure 8.3A linearly polarised electromagnetic wave, propagating in the z-direction with the oscillating electric field E along the x-direction and the oscillating magnetic field B along the y-direction.
Fig. 8.3 — A linearly polarised electromagnetic wave, propagating in the z-direction with the oscillating electric field E along the x-direction and the oscillating magnetic field B along the y-direction.

Drawn by us to help you understand the concept clearly, and verified to make sure it's accurate. For exams, practice from your textbook's own diagram.

What the Figure Shows

The figure is a 3‑axis perspective sketch of a plane electromagnetic wave.

  • The z‑axis runs horizontally to the right — this is the direction of propagation of the wave.
  • The x‑axis points vertically upward.
  • The y‑axis is drawn down‑left in perspective, so all three axes are mutually perpendicular.

Two sinusoidal curves are drawn along the z‑axis:

  1. Electric field E\mathbf{E}: a sine wave lying in the vertical x–z plane. Small vertical arrows along the curve show that E\mathbf{E} oscillates along the x‑direction. The first crest is labelled E and points along +x+x.
  2. Magnetic field B\mathbf{B}: a sine wave of the same wavelength and phase lying in the horizontal y–z plane. Arrows along the curve show that B\mathbf{B} oscillates along the y‑direction. The first crest is labelled B and points along +y+y.

Both sine curves share the z‑axis, are in phase (crest‑to‑crest, trough‑to‑trough), and are transverse — their oscillations are perpendicular to the propagation direction zz.


The Physical Idea

The figure illustrates three essential properties of a plane electromagnetic wave in free space:

  • Mutual perpendicularity: E\mathbf{E} is along xx, B\mathbf{B} is along yy, and the wave travels along zz. Each field is perpendicular to the other two directions.
  • Transverse nature: Both E\mathbf{E} and B\mathbf{B} oscillate perpendicular to the direction of propagation.
  • Same phase: The electric and magnetic fields reach their maxima and minima together — they are in phase, not out of phase.

This is a linearly polarised wave because the electric field oscillates along a fixed line (the x‑axis).


Key Formulas Developed from This Figure

From the sinusoidal variation shown in the figure, the textbook writes the fields as:

Ex=E0sin⁡(kz−ωt)E_x = E_0 \sin(kz - \omega t)

By=B0sin⁡(kz−ωt)B_y = B_0 \sin(kz - \omega t)

  • ExE_x: electric field component along the x‑axis
  • ByB_y: magnetic field component along the y‑axis
  • E0E_0, B0B_0: amplitudes of the electric and magnetic fields
  • k=2πλk = \frac{2\pi}{\lambda}: wave number (magnitude of the propagation vector k\mathbf{k}) …