theorem

Poynting's theorem

Poynting's theorem expresses the conservation of energy for electromagnetic fields in terms of power flow and dissipation.
11 related articles · 3 formulas

Description

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.

History

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.

How it works

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.

Fun fact

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!

Concept graph →

Formulas

$$\frac{dN}{dE} \propto E^{-\alpha} \exp(-E/E_{\mathrm{cut}})$$
Particle energy spectrum with power law and exponential cutoff.
What is in the formula
dN/dEvariableDifferential number of particles per energy interval — particle spectrum joule per joule
EvariableParticle energy — energy joule
alphavariableSpectral index of the power law
E_cutvariableCutoff energy — energy joule
\frac{dn}{de}\proptoe^{-α}\exp(-e/e_{{cut}}) · 2606.06974v1
$$V(z) = \phi - eFz - \frac{e^2}{4\pi\epsilon_0 z}$$
Potential energy for electron emission including work function and field.
What is in the formula
Vvariablepotential energy of electron — potential energy joule
zvariabledistance from the metal surface — position metre
φvariablework function of the metal — work function joule
Fvariableapplied electric field strength — electric field volt per metre
econstantcharge of a single proton — elementary charge = 1.602176634e-19 coulomb
ε0constantability of vacuum to permit electric field lines — vacuum permittivity = 8.8541878128e-12 farad per metre
m(φ,f,z)=φ-efz-\frac{e^{2}}{16πε_{0}z} · 2505.00872v4
$$F_{\text{total}} = \sigma T^4$$
Total flux equals Stefan-Boltzmann radiation.
What is in the formula
F_{\text{total}}variabletotal radiative flux emitted per unit area — radiative flux watt per square metre
Tvariableabsolute temperature of the radiating body — temperature kelvin
\sigmaconstantStefan-Boltzmann constant relating temperature to radiated power — stefan boltzmann constant = 5.670374419e-8 watt per square metre per kelvin to the fourth
f_{\rmrad}+f_{\rmconv}=σ_{\rmsb}t_{\rmeff}^4 · 2607.24141v1

Related articles · 12

Mesoscale2026-06-263 minarXiv:2606.27788
Spaghetti in Soup: How Fractional Vortices Make Superfluidity Melt Twice
Two-dimensional worlds never cease to amaze: here even crystal melting is not a symmetry breaking but a vortex drama discovered by Kosterlitz and Thouless. At the heart of this theater are topological сингулярности, whose energy and энтропия bargain for order. This language is common to сверхтекучести и сверхпроводимости.
General Relativity2026-06-151 minarXiv:2606.16680express
How the Universe Got Magnetized Before the First Stars
Right after the Big Bang, space was a hot plasma — a mix of charged particles and light. In such a medium, electric currents couldn't flow on their own: a 'potential difference' was needed to push electrons relative to photons.
Cosmology2026-06-031 minarXiv:2606.04886express
Dark energy may be losing energy: explaining strange behavior
In the late 1990s, astronomers including Saul Perlmutter discovered that the universe is expanding at an accelerating rate. The cause was dubbed dark energy — an invisible force stretching the cosmos.
HEP Phenomenology2026-05-202 minarXiv:2605.21281express
Magnetic Hunters for Galaxies
An ordinary magnet always carries two poles — north and south. Split it in half, and each piece immediately grows its own pair. But deep in particle theory lives a strange notion: the monopole — a particle carrying just one magnetic charge, a lone pole without a partner.
Mesoscale2026-05-102 minarXiv:2605.09488express
Dark Excitons: A Quantum Trickle in a Chip
In a thin sandwich of semiconductors, light creates pairs, an electron and a positive hole, that stick together like a ball on a rubber band. Normally, such pairs, called excitons, quickly emit light and vanish. But there are others, dark ones, that live hundreds of times longer because their internal structure forbids them from easily giving off energy.
General Relativity2026-04-302 minarXiv:2604.27575express
Energy in a Gravitational Field: Almost Like Water in a Pipe
If you pour sand into a glass, it settles in a flat layer. But instead of sand, take the tiniest particles of gas: in a gravitational field they don't just fall: each particle races along its own trajectory, collides with neighbors, and all this commotion creates pressure.
Nuclear Experiment2026-04-271 minarXiv:2604.24220express
Stretching a Deuterium Nucleus with Light
A drop of water stretches in a strong electric field. The deuterium nucleus, a bound pair of a proton and a neutron, behaves the same way, except here the field comes from a passing gamma ray, and instead of just stretching, the nucleus can simply fall apart.
Nuclear Experiment2026-04-161 minarXiv:2604.15546express
Why the Proton 'Lost Weight' and Then 'Gained It Back'
To uncover the proton's true size, physicists swapped the electron in a hydrogen atom for its heavy copy — the muon. Acting like a magnifying glass with thousandfold power, the muon gets right up against the nucleus and 'probes' the proton with unprecedented precision.
Quantum Physics2026-01-092 minarXiv:2601.05514express
A Wire Heats Up from Knowledge
Run a current through a wire, and the wire heats up. Anyone who has ever touched a phone charger knows this. Physicists call this heating Joule heating, after James Joule, who in the mid-19th century measured how much heat electricity produces. Since then, the formula has been simple: the greater the resistance and the current, the hotter the wire.
Fluid Dynamics2026-01-042 minarXiv:2601.01476express
Invisible Waves in the Ocean's Depths
The ocean is like a layered cake: warm, light water on top, cold, heavy water below. Between the layers, at the interface, invisible waves roam. They don't lift crests like a storm; instead, they slowly rock the entire water column, as if someone were shaking a giant aquarium from within.
Pilot Photons: Relativistic Bohmian Mechanics Seen Directly
A single photon passes through two slits and leaves an interference pattern on a screen. Quantum mechanics describes this process with a wave function, but what happens to the particle itself?