Electron: Difference between revisions
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::''μ<sub>B</sub>'' = 927.400 915 x 10<sup>-26</sup> J/ T. | ::''μ<sub>B</sub>'' = 927.400 915 x 10<sup>-26</sup> J/ T. | ||
Together with [[neutron]]s and [[proton]]s in atomic [[nucleus (physics)|nuclei]], electrons constitute [[atom]]s and [[molecule]]s. The (quantum mechanical) interaction between electrons on nearby atoms underlies the [[chemical bonding]] in molecules, gases, liquids and solids, such as [[crystals]]. The statistical behavior of large numbers of electrons is governed by the [[Fermi function]]. | |||
The behavior of electrons at the microscopic level of individual particles or atoms must be described by [[quantum mechanics]] or [[quantum electrodynamics]]. On a larger scale, however, these microscopic considerations often can be approximated as macroscopic currents and charges, which then are used in [[classical electrodynamics]] to describe [[electromagnetic fields]] using the (classical) [[Maxwell equations]]. In such an approach, quantum mechanics can be used to establish the electronic properties of materials, which then are expressed in the macroscopic Maxwell equations by introducing material parameters such as permittivities, permeabilities, conductivities and the like without further need for quantum theory. | |||
==References== | ==References== | ||
<references/> | <references/> | ||
Revision as of 13:25, 30 March 2011
An electron is an elementary particle that carries a negative elementary charge −e.[1]
- e = 1.602 176 487 × 10-19 C
It is a spin-½ lepton of mass[2]
- me= 9.109 382 15 × 10−31 kg.
It has a gyromagnetic ratio[3]
- γe = 1.760 859 770 x 1011 s-1 T-1
or a magnetic moment of about −1.00115965 Bohr magneton (μB):[4]
- μB = 927.400 915 x 10-26 J/ T.
Together with neutrons and protons in atomic nuclei, electrons constitute atoms and molecules. The (quantum mechanical) interaction between electrons on nearby atoms underlies the chemical bonding in molecules, gases, liquids and solids, such as crystals. The statistical behavior of large numbers of electrons is governed by the Fermi function.
The behavior of electrons at the microscopic level of individual particles or atoms must be described by quantum mechanics or quantum electrodynamics. On a larger scale, however, these microscopic considerations often can be approximated as macroscopic currents and charges, which then are used in classical electrodynamics to describe electromagnetic fields using the (classical) Maxwell equations. In such an approach, quantum mechanics can be used to establish the electronic properties of materials, which then are expressed in the macroscopic Maxwell equations by introducing material parameters such as permittivities, permeabilities, conductivities and the like without further need for quantum theory.
References
- ↑ Elementary charge. The NIST reference on constants, units, and uncertainty. National Institute of Standards and Technology. Retrieved on 2011-03-28.
- ↑ Electron mass. The NIST reference on constants, units, and uncertainty. Retrieved on 2011-03-28.
- ↑ Electron gyromagnetic ratio. The NIST reference on constants, units, and uncertainty. Retrieved on 2011-03-28.
- ↑ Bohr magneton. The NIST reference on constants, units, and uncertainty. Retrieved on 2011-03-28.