Electron mass energy equivalent
| Value | 8.187105788e-14 J |
| Status | Measured: ± 2.60e-23 J (3.2e-10 relative) |
| Source | CODATA 2022 |
| Categories | Universal & Atomicphysicsnuclear |
| joule | 8.1871058e-14 J |
| kilojoule | 8.1871058e-17 kJ |
| megajoule | 8.1871058e-20 MJ |
| calorie | 1.9567652e-14 cal |
| kilocalorie | 1.9567652e-17 kcal |
| watt-hour | 2.2741961e-17 Wh |
| kilowatt-hour | 2.2741961e-20 kWh |
| British thermal unit | 7.7598790e-17 BTU |
| foot-pound | 6.0384993e-14 ft⋅lb |
| electron volt | 510,998.95 eV |
| kiloelectron volt | 510.99895 keV |
| megaelectron volt | 0.51099895 MeV |
Learning zone
511 keV is one of the most recognisable numbers in physics. When a positron meets an electron the pair annihilates into two photons of exactly this energy flying back-to-back, which is what a PET scanner's detector ring times to milimetre precision, and what gamma-ray telescopes see glowing from the centre of the Milky Way.
It also sets thresholds. Pair production from a single photon needs at least 2m_e c² = 1.022 MeV plus a nucleus to absorb the recoil, so no gamma below 1.022 MeV can make an electron-positron pair. And it marks the boundary of relativity for electrons: a 511 keV kinetic energy means γ = 2, so anything in a linac or a CRT beyond a few tens of keV already needs relativistic kinematics, while thermal electrons at 0.025 eV are hopelessly non-relativistic.