Electron: Difference between revisions
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An '''electron''' is an [[elementary particle]] that carries a negative [[elementary charge]] −''e''. It is a [[electron spin|spin-½]] [[lepton]] of mass 9.109 382 15 × 10<sup>−31</sup> kg. Because of this small mass the motion of an electron must often be described by [[quantum mechanics]] or [[quantum electrodynamics]]. However, [[classical electrodynamics]], describing the behavior of electrons in [[electromagnetic fields]] by the (classical) [[Maxwell equations]], has | An '''electron''' is an [[elementary particle]] that carries a negative [[elementary charge]] −''e''. It is a [[electron spin|spin-½]] [[lepton]] of mass 9.109 382 15 × 10<sup>−31</sup> kg. Because of this small mass the motion of an electron must often be described by [[quantum mechanics]] or [[quantum electrodynamics]]. However, [[classical electrodynamics]], describing the behavior of electrons in [[electromagnetic fields]] by the (classical) [[Maxwell equations]], still has its use in [[electrical engineering]] and many branches of [[physics]]. Together with atomic [[nucleus (physics)|nuclei]], electrons constitute [[atom]]s and [[molecule]]s. Their (quantum mechanical) interaction with adjacent nuclei causes [[chemical bonding]] and bonding in [[crystals]]. | ||
==References== | ==References== | ||
<references/> | <references/> | ||
Revision as of 20:40, 18 January 2011
An electron is an elementary particle that carries a negative elementary charge −e. It is a spin-½ lepton of mass 9.109 382 15 × 10−31 kg. Because of this small mass the motion of an electron must often be described by quantum mechanics or quantum electrodynamics. However, classical electrodynamics, describing the behavior of electrons in electromagnetic fields by the (classical) Maxwell equations, still has its use in electrical engineering and many branches of physics. Together with atomic nuclei, electrons constitute atoms and molecules. Their (quantum mechanical) interaction with adjacent nuclei causes chemical bonding and bonding in crystals.