- Energy-momentum relation
In
special relativity , the energy-momentum relation is a relation between theenergy ,momentum and themass of a body::where "c" is thespeed of light , is total energy, is invariant mass, and is momentum.For a body in its rest frame, the momentum is zero, so the equation simplifies to:If the object is massless then the energy momentum relation reduces to:as is the case for a
photon .In
natural units the energy-momentum relation can be expressed as:where isangular frequency , is rest mass and iswave number .In
Minkowski space , energy and momentum (the latter multiplied by a factor of c) can be seen as two components of a Minkowskifour-vector . The norm of this vector is equal to the square of the rest mass of the body, which is aLorentz invariant quantity and hence is independent of theframe of reference .When working in units where "c" = 1, known as the
natural unit system , the energy-momentum equation reduces to:In
particle physics , energy is typically given in units ofelectron volt s (eV), momentum in units of eV/c, and mass in units of eV/c2. In electromagnetism, and because of relativistic invariance, it is useful to have the electric field E and the magnetic field B in the same unit (gauss), using the cgs (gaussian) system of units, where energy is given in units oferg , momentum in g.cm/s and mass ingram s.Energy may also in theory be expressed in units of grams, though in practice it requires a large amount of energy to be equivalent to masses in this range. For example, the first atomic bomb liberated about 1 gram of heat, and the largest thermonuclear bombs have generated a kilogram or more of heat. Energies of thermonuclear bombs are usually given in tens of kilotons and megatons referring to the energy liberated by exploding that amount of
trinitrotoluene (TNT).ee also
*
Mass-energy equivalence
*Four-momentum
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