Planck charge

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In physics, the Planck charge, denoted by q_{{\text{P}}}, 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 defined as:[1] [2]

q_{{\text{P}}}={\sqrt  {4\pi \epsilon _{0}\hbar c}}={\sqrt  {2ch\epsilon _{0}}}={\frac  {e}{{\sqrt  {\alpha }}}}=1.875\;5459\times 10^{{-18}} coulombs,

where:

c\ is the speed of light in the vacuum,
h\ is Planck's constant,
\hbar \equiv {\frac  {h}{2\pi }}\ is the reduced Planck constant,
\epsilon _{0}\ is the permittivity of free space
e\ is the elementary charge
\alpha \ = (137.03599911)1 is the fine structure constant.

The Planck charge is \alpha ^{{-1/2}}\approx 11.706 times greater than the elementary charge e carried by an electron.

The Gaussian cgs units are defined so that 4\pi \epsilon _{0}=1, in which case q_{{\text{P}}} has the following simple form:

q_{{\text{P}}}={\sqrt  {\hbar c}}.

It is customary in theoretical physics to adopt the Lorentz–Heaviside units (also known as rationalized cgs). When made natural (c=1) they are like the SI system with \epsilon _{0}=\mu _{0}=1. Therefore it is more appropriate to define the Planck charge as

q'_{{\text{P}}}={\sqrt  {\epsilon _{0}\hbar c}}={\frac  {e}{{\sqrt  {4\pi \alpha }}}}=5.291\times 10^{{-19}} coulombs,

When charges are measured in units of q'_{{\text{P}}}, i.e., when q'_{{\text{P}}} is set equal to 1, we obtain \alpha =e^{2}/(4\pi ), which is commonly used in theoretical physics. In contrast, in (non-rationalized) natural cgs units where q_{{\text{P}}}=1 we have \alpha =e^{2}.

See also

Notes and references

  1. 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. 
  2. Pavšič, Matej (2001). The Landscape of Theoretical Physics: A Global View. Dordrecht: Kluwer Academic. pp. 347–352. ISBN 0-7923-7006-6. 
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