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Radio, television, mobile networks, Wi-Fi, microwave ovens, X-ray machines and even sunlight are all electromagnetic waves. They differ from one another only in frequency (wavelength). In this topic we see how such a wave arises, its properties, the electromagnetic spectrum, and the principles of radio communication and radar.
Maxwell (1864) combined two ideas:
So once changing fields appear, they keep generating each other and travel through space — this is an electromagnetic wave. It is emitted by accelerating charges (for example, electrons oscillating in an antenna). A closed LC circuit hardly radiates, so an antenna is an open circuit. Hertz was the first to produce and detect such waves experimentally (1888).
From his equations Maxwell calculated the speed of the wave: c = 1/√(ε₀μ₀) ≈ 3·10⁸ m/s. This matched the measured speed of light, and Maxwell concluded that light is an electromagnetic wave too. Hertz, using a spark-gap dipole and a receiving loop (resonator), showed that the waves reflect, refract and form standing waves, and confirmed that they travel at the speed of light.
c = 3·10⁸ m/s
The basic relation:
c = λν, λ = cT
When a wave enters another medium its frequency does not change; the speed and wavelength change: λ_medium = λ₀/n.
An FM station broadcasts at 100 MHz. Wavelength?
Light with a vacuum wavelength of 600 nm enters glass (n = 1.5). Speed and wavelength in the glass?
In a closed circuit the electric field is “locked” inside the capacitor and the magnetic field inside the coil, so it hardly radiates. If we pull the capacitor plates apart and straighten the coil into a wire, we get an open circuit, a dipole (aerial): the field fills the surrounding space and breaks away as a wave. The simplest aerial is a wire half a wavelength long (a half-wave dipole), in which the current oscillations build up by resonance. That is why aerials for high frequencies (mobile phones, Wi-Fi) are small, while long-wave radio masts are very tall.
An electromagnetic wave carries energy equally in its electric and magnetic fields. From the quantum point of view radiation is a stream of photons, each with energy
E = hν = hc/λ, h = 6.63·10⁻³⁴ J·s
The shorter the wavelength, the greater the photon energy. Ultraviolet, X-rays and gamma rays can break bonds in molecules, so they are ionising radiation, whereas radio photons are far too weak for that.
Find the length of a half-wave aerial for 100 MHz and the energy of one photon.
In order of decreasing wavelength and increasing frequency:
As frequency increases, the photon energy (E = hν) and penetrating power increase.
Sound frequencies (20 Hz – 20 kHz) are low, and such waves cannot be radiated efficiently. Therefore:
Among the first to use radio in practice were A. S. Popov (1895) and G. Marconi.
A radar sends a short pulse and receives the signal reflected from an object. The signal covers the distance twice:
s = ct/2
The gap between pulses must be longer than the echo’s return time, so the maximum range is s_max = c/(2ν_pulse).
A radar echo returns after 200 μs. Distance to the object?
The distance to the Moon is 3.84·10⁸ m. After what time does a radio echo return?
Intensity is the energy a wave carries per second through 1 m² of a perpendicular surface (W/m²). For a point source radiating equally in all directions:
I = P/(4πr²)
Doubling the distance cuts the intensity by a factor of 4. The intensity radiated by an oscillating charge is proportional to the fourth power of frequency (ν⁴) — this is why radio uses a high-frequency carrier.
Intensity 10 m from a 100 W source?