Larmor theorem in classical electrodynamics
E811516
The Larmor theorem in classical electrodynamics states that a charged particle in a weak, uniform magnetic field behaves as if it were in a rotating reference frame, leading to a characteristic precession of its orbital motion at the Larmor frequency.
Observed surface forms (1)
| Surface form | Occurrences |
|---|---|
| Larmor theorem | 0 |
Statements (47)
| Predicate | Object |
|---|---|
| instanceOf |
physical theorem
ⓘ
result in classical electrodynamics ⓘ |
| appliesTo |
charged particle in a uniform magnetic field
ⓘ
charged particle in a weak magnetic field ⓘ |
| assumes |
absence of electric field or slowly varying electric field
ⓘ
nonrelativistic motion ⓘ uniform magnetic field ⓘ weak magnetic field limit ⓘ |
| category |
classical mechanics and electrodynamics interface
ⓘ
electromagnetism theorem ⓘ |
| connects | magnetic field strength with angular velocity of precession ⓘ |
| countryOfOrigin | United Kingdom ⓘ |
| defines | Larmor frequency NERFINISHED ⓘ |
| describes |
motion of charged particles in magnetic fields
ⓘ
precession of the plane of a charged particle’s orbit ⓘ |
| era | late 19th century physics ⓘ |
| field | classical electrodynamics ⓘ |
| holdsIn | classical limit of electrodynamics ⓘ |
| implies | equivalence between weak uniform magnetic field and rotating frame for orbital motion ⓘ |
| influenced | development of quantum mechanical treatment of magnetic interactions ⓘ |
| involvesConcept | equivalence principle for magnetic field and rotation (in weak-field limit) ⓘ |
| involvesQuantity |
angular velocity of precession
ⓘ
charge q ⓘ magnetic field B ⓘ mass m ⓘ |
| isAnalogousTo | Larmor precession of quantum mechanical spin ⓘ |
| mathematicalForm |
ω_L = −(q B)/(2 m c) in Gaussian units for orbital motion
ⓘ
ω_L = −(q B)/(2 m) in SI units for orbital motion without c factor ⓘ |
| namedAfter | Joseph Larmor NERFINISHED ⓘ |
| predicts |
Larmor precession
NERFINISHED
ⓘ
precession of orbital motion of a charged particle ⓘ |
| relatedConcept |
Larmor frequency
NERFINISHED
ⓘ
Larmor precession NERFINISHED ⓘ Lorentz force NERFINISHED ⓘ Zeeman effect NERFINISHED ⓘ gyromagnetic ratio ⓘ magnetic moment precession ⓘ orbital angular momentum in a magnetic field ⓘ rotating reference frame ⓘ |
| relates | magnetic field to effective rotating reference frame ⓘ |
| states | a charged particle in a weak uniform magnetic field behaves as if in a rotating frame ⓘ |
| usedFor |
deriving Larmor precession of magnetic moments
ⓘ
describing orbital precession in atoms ⓘ relating magnetic field to precession frequency of angular momentum ⓘ understanding Zeeman effect qualitatively ⓘ |
| validWhen |
magnetic field varies slowly in space
ⓘ
magnetic field varies slowly in time ⓘ |
Referenced by (1)
Full triples — surface form annotated when it differs from this entity's canonical label.