Proton mass energy equivalent
| Value | 1.50327761802e-10 J |
| Status | Measured: ± 5.20e-20 J (3.5e-10 relative) |
| Source | CODATA 2022 |
| Categories | Universal & AtomicNuclear |
| electron volt | 938,272,090 eV |
| hartree | 34,480,863 Eh |
| kiloelectron volt | 938,272.09 keV |
| megaelectron volt | 938.27209 MeV |
| gigaelectron volt | 0.93827209 GeV |
| nanojoule | 0.15032776 nJ |
| erg | 0.0015032776 erg |
| teraelectron volt | 0.00093827209 TeV |
| microjoule | 0.00015032776 µJ |
| millijoule | 1.5032776e-07 mJ |
| inch-pound | 1.3305128e-09 in·lb |
| joule | 1.5032776e-10 J |
| foot-pound | 1.1087607e-10 ft⋅lb |
| calorie | 3.5929197e-11 cal |
| calorie (International Table) | 3.5905169e-11 cal IT |
| kilojoule | 1.5032776e-13 kJ |
| BTU (thermochemical) | 1.4257858e-13 BTU th |
| British thermal unit | 1.4248323e-13 BTU |
| watt-hour | 4.1757712e-14 Wh |
| kilocalorie | 3.5929197e-14 kcal |
| megajoule | 1.5032776e-16 MJ |
| horsepower-hour | 5.5998014e-17 hp·h |
| kilowatt-hour | 4.1757712e-17 kWh |
| therm | 1.4248323e-18 therm |
| gigajoule | 1.5032776e-19 GJ |
| million BTU | 1.4248323e-19 MMBTU |
| megawatt-hour | 4.1757712e-20 MWh |
| ton of TNT | 3.5929197e-20 t TNT |
| tonne of oil equivalent | 3.5905169e-21 toe |
| terajoule | 1.5032776e-22 TJ |
| gigawatt-hour | 4.1757712e-23 GWh |
| kiloton of TNT | 3.5929197e-23 kt TNT |
| petajoule | 1.5032776e-25 PJ |
| terawatt-hour | 4.1757712e-26 TWh |
| megaton of TNT | 3.5929197e-26 Mt TNT |
| quad | 1.4248323e-28 quad |
Learning zone
938.272 MeV is the reference mass of nuclear and particle physics. A proton beam is called relativistic once its kinetic energy approaches this figure; at the LHC each proton carries 6.8 TeV, roughly 7250 times its own rest energy, so γ ≈ 7250 and the beam travels within 3 m/s of c. Proton therapy beams, by contrast, run at 70–250 MeV — still under a third of the rest energy, yet enough to place a Bragg peak inside a tumour.
The nucleon mass also fixes the scale of everything heavier: a nucleus of mass number A weighs roughly A × 939 MeV/c² minus about 8 MeV per nucleon of binding. That 8-in-939 shortfall — under 1 % — is the entire energy supply of both fission reactors and stars, which is a fair measure of how much energy c² packs into a tiny fractional mass change.