Planck charge
In physics, the Planck charge, denoted by , is one of the base units in the system of natural units called Planck units. It is a quantity of electric charge defined in terms of fundamental physical constants.
The Planck charge is the only base Planck unit that does not depend on the gravitational constant; it is defined as[1][2]
where
- is the speed of light in vacuum
- is the reduced Planck constant
- is the permittivity of free space
- is the elementary charge
- is the fine structure constant.
From a classical calculation,[3] the electric potential energy of one Planck charge on the surface of a sphere that is one Planck length in diameter is one Planck energy,
In other words, the energy required to accumulate one Planck charge on a sphere one Planck length in diameter will make the sphere one Planck mass heavier,
where
- is the Coulomb constant
- is the speed of light
- is the Planck energy
- is the Planck charge
- is the Planck length
- is the Planck mass
Rationalized units: If, instead, a rationalized form of Planck units is chosen, in which units are defined in terms of ℏ, c and without numerical factors, the resulting rationalized Planck charge is
When charges are measured in units of , used in quantum field theory, one has
- .
Physical significance
The Planck charge is the maximum amount of charge that a black hole the size of one Planck length can possess, and adding more charge would make the black hole inevitably larger. In particular, Reissner–Nordström metric (the solution for a non-rotating charged black hole) tends to the Planck length for a mass that tends to zero and a charge that equals the Planck charge.
Notes and references
- ^ Stock, Michael; Witt, Thomas J (2006). "CPEM 2006 round table discussion 'Proposed changes to the SI'". Metrologia. 43 (6): 583. Bibcode:2006Metro..43..583S. doi:10.1088/0026-1394/43/6/014.
- ^ Pavšič, Matej (2001). The Landscape of Theoretical Physics: A Global View. Dordrecht: Kluwer Academic. pp. 347–352. arXiv:gr-qc/0610061. ISBN 0-7923-7006-6.
- ^ The Feynman Lectures on Physics, Volume II, ch. 8: Electrostatic Energy