Nuclear magneton







Nuclear magneton





Nuclear magneton

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The nuclear magneton (symbol \mu_\mathrm{N}\!), is a physical constant of magnetic moment, defined by:

\mu_\mathrm{N} = {{e \hbar} \over {2 m_\mathrm{p}}}

where:

e\! is the elementary charge,
\hbar is the reduced Planck's constant,
m_\mathrm{p}\! is the proton rest mass

In the SI system of units its value is approximately:

\mu_\mathrm{N}\! = 5.050 783 24(13) í— 10-27 J·T-1

The nuclear magneton is the natural unit for expressing magnetic dipole moments of heavy particles such as nucleons and atomic nuclei. On the countrary, the dipole moment of the electron, which is much higher as a consequence of much higher charge-to-mass ratio, is usually expressed in corresponding units of the Bohr magneton.

See also

External links


Nuclear magneton


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