
Poynting's theorem expresses the conservation of energy for electromagnetic fields in terms of power flow and dissipation.Sunlight carries energy across the void of space. Poynting's theorem reveals the balance: the energy of the electromagnetic field doesn't disappear, but either leaves across an imaginary boundary of a volume or heats the charges inside. Poynting presented the energy flow as a vector, always perpendicular to the electric and magnetic fields — like the direction of wind blowing leaves away.
In 1884, John Henry Poynting, building on James Clerk Maxwell's equations, derived a relation showing that the energy of the electromagnetic field is transferred not along wires, but through the surrounding space. He introduced the concept of the energy flux vector, later named after him. Oliver Heaviside independently reached similar conclusions. The theorem became a cornerstone of radiation theory and the foundation for all modern radio electronics.
The theorem is applied in the design of antennas, waveguides, fiber-optic lines, and electromagnetic compatibility analysis. It holds rigorously for classical fields, and in quantum electrodynamics is generalized via energy operators. Limits of applicability: situations where radiation from accelerated charges or hysteresis of the medium are neglected.
If you point an antenna at a blank wall, the energy of radio waves reflects back, and the Poynting vector turns around. And in a microwave oven, this vector points straight into your food!
| dN/dE | variable | Differential number of particles per energy interval — particle spectrum joule per joule |
| E | variable | Particle energy — energy joule |
| alpha | variable | Spectral index of the power law |
| E_cut | variable | Cutoff energy — energy joule |
| V | variable | potential energy of electron — potential energy joule |
| z | variable | distance from the metal surface — position metre |
| φ | variable | work function of the metal — work function joule |
| F | variable | applied electric field strength — electric field volt per metre |
| e | constant | charge of a single proton — elementary charge = 1.602176634e-19 coulomb |
| ε0 | constant | ability of vacuum to permit electric field lines — vacuum permittivity = 8.8541878128e-12 farad per metre |
| F_{\text{total}} | variable | total radiative flux emitted per unit area — radiative flux watt per square metre |
| T | variable | absolute temperature of the radiating body — temperature kelvin |
| \sigma | constant | Stefan-Boltzmann constant relating temperature to radiated power — stefan boltzmann constant = 5.670374419e-8 watt per square metre per kelvin to the fourth |






