rdf:type |
qudt:PhysicalConstant |
dcterms:description |
The \(\textit{Electron Gyromagnetic Ratio}\) is a property that an isolated electron has for its angular momentum and magnetic moment resulting from its spin.
While an electron's spin is sometimes visualized as a literal rotation about an axis, it is in fact a fundamentally different, quantum-mechanical phenomenon with no true analogue in classical physics.
As a consequence there is no reason to expect the above classical relation to hold.
|
qudt:applicableUnit |
unit:A-M2-PER-J-SEC |
qudt:hasQuantityKind |
quantitykind:GyromagneticRatio |
qudt:informativeReference |
|
qudt:isoNormativeReference |
http://www.iso.org/iso/catalogue_detail?csnumber=31895 |
qudt:latexDefinition |
\(\mu = \gamma_e J\), where \(\mu\) is the magnetic dipole moment, and \(J\) is the total angular momentum. |
qudt:latexSymbol |
\(\gamma_e\) |
qudt:normativeReference |
http://www.iso.org/iso/catalogue_detail?csnumber=31895 |
qudt:quantityValue |
constant:Value_ElectronGyromagneticRatio |
rdfs:isDefinedBy |
http://qudt.org/3.1.10/vocab/constant |
rdfs:label |
“Electron Gyromagnetic Ratio”@en |
skos:closeMatch |
http://dbpedia.org/resource/Gyromagnetic_ratio |
