The simplest source studied by Hertz is the dipole antenna: a length of conducting wire of length fed at its centre by an alternating generator that makes the current oscillate at frequency . For a dipole that radiates efficiently, the optimal length is , with the associated wavelength.
Vertical dipole antenna: the alternating generator at the centre makes the current oscillate; the wave fronts radiate outwards concentrically.
Far from the antenna (far field, ) the magnitude of the wave decreases as , so the intensity decreases as — as for an isotropic point source, but with a torus-shaped directionality: maximum in the equatorial plane, zero along the dipole’s axis. The polarisation of the emitted electric field is parallel to the antenna’s axis: a vertical antenna emits waves with vertical.
Example — FM and WiFi antennas
An FM radio station at MHz has m: an optimal dipole is about m long, exactly the size typically seen on masts. WiFi at GHz has cm: the antenna is about cm long and fits entirely inside the router. A mobile phone at GHz ( cm) has an antenna a couple of centimetres long. It is always the same physics: everything is fixed by the wavelength (Bloomfield 2016).
Tesla's "wireless light bulb"
In 1891 Nikola Tesla showed gas tubes that lit up in his hand without wires: the EM field of a high-frequency coil ionised the gas at a distance. The same idea is exploited today by the wireless charging of smartphones: an antenna in the base generates an oscillating magnetic field that induces a current in a receiving antenna inside the phone’s casing — a miniature version of Hertz’s experiment.
In summary
Accelerated charge EM wave. Dipole antenna of length , with parallel to the axis and intensity .
Links
Topics: Electromagnetic waves Concepts: Electromagnetic wave · Polarisation and Malus’s law · Intensity of a wave
Related exercises: Problem — TV antennas and polarisation · Problem — Crossed polarisers · Problem — Crossed polarisers with one in between