Richardson–Dushman equation
E835820
The Richardson–Dushman equation is a fundamental formula in thermionic emission theory that relates the current density of electrons emitted from a heated metal surface to its temperature and material-specific constants.
All labels observed (1)
| Label | Occurrences |
|---|---|
| Richardson–Dushman equation canonical | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T10003219 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
Target entity: Richardson–Dushman equation Context triple: [Edison effect, relatedTo, Richardson–Dushman equation]
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A.
Butler–Volmer equation
The Butler–Volmer equation is a fundamental relation in electrochemistry that describes how the rate of an electrode reaction (current density) depends on the electrode potential and reaction kinetics.
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B.
Nernst–Planck equation
The Nernst–Planck equation is a fundamental relation in electrochemistry that describes the flux of charged species under the combined influence of diffusion, electric fields, and, in extended forms, convection.
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C.
Randles–Ševčík equation
The Randles–Ševčík equation is a fundamental electrochemical relationship that links peak current in cyclic voltammetry to the concentration and diffusion coefficient of a redox-active species.
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D.
Fick's first law of diffusion
Fick's first law of diffusion is a fundamental physical law that relates the diffusive flux of particles to the spatial gradient of their concentration, describing how substances move from regions of high to low concentration.
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E.
Bhabha–Corben equations
The Bhabha–Corben equations are relativistic wave equations in quantum electrodynamics that describe the dynamics of spinning charged particles, developed by physicists Homi J. Bhabha and H. C. Corben.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Richardson–Dushman equation Target entity description: The Richardson–Dushman equation is a fundamental formula in thermionic emission theory that relates the current density of electrons emitted from a heated metal surface to its temperature and material-specific constants.
-
A.
Butler–Volmer equation
The Butler–Volmer equation is a fundamental relation in electrochemistry that describes how the rate of an electrode reaction (current density) depends on the electrode potential and reaction kinetics.
-
B.
Nernst–Planck equation
The Nernst–Planck equation is a fundamental relation in electrochemistry that describes the flux of charged species under the combined influence of diffusion, electric fields, and, in extended forms, convection.
-
C.
Randles–Ševčík equation
The Randles–Ševčík equation is a fundamental electrochemical relationship that links peak current in cyclic voltammetry to the concentration and diffusion coefficient of a redox-active species.
-
D.
Fick's first law of diffusion
Fick's first law of diffusion is a fundamental physical law that relates the diffusive flux of particles to the spatial gradient of their concentration, describing how substances move from regions of high to low concentration.
-
E.
Bhabha–Corben equations
The Bhabha–Corben equations are relativistic wave equations in quantum electrodynamics that describe the dynamics of spinning charged particles, developed by physicists Homi J. Bhabha and H. C. Corben.
- F. None of above. chosen
Statements (48)
| Predicate | Object |
|---|---|
| instanceOf |
equation
ⓘ
physical law ⓘ |
| alsoKnownAs |
Richardson equation
NERFINISHED
ⓘ
Richardson–Dushman law NERFINISHED ⓘ |
| appliesTo |
electron emission from heated cathodes
ⓘ
electron emission from heated metal surfaces ⓘ |
| assumes |
clean metal surface
ⓘ
no space-charge limitation ⓘ thermally equilibrated electron gas in metal ⓘ |
| canBeModifiedBy | Schottky correction for electric field ⓘ |
| category |
electron emission theory
ⓘ
statistical mechanics applications ⓘ |
| dependsOn |
Boltzmann constant
NERFINISHED
ⓘ
absolute temperature ⓘ material work function ⓘ |
| derivedFrom |
Fermi–Dirac statistics
NERFINISHED
ⓘ
classical emission over a potential barrier ⓘ |
| describes | thermionic emission current density ⓘ |
| domainOfValidity | high-temperature operation of metals ⓘ |
| field |
solid-state physics
ⓘ
surface physics ⓘ thermionic emission ⓘ vacuum electronics ⓘ |
| hasHistoricalSignificance | foundation of early vacuum tube theory ⓘ |
| hasMathematicalForm | J = A T^2 exp(-\phi / k_B T) ⓘ |
| hasUnitForJ | ampere per square meter ⓘ |
| ignores | Schottky effect unless modified ⓘ |
| includesParameter |
Richardson constant
NERFINISHED
ⓘ
metal work function ⓘ |
| namedAfter |
Irving Langmuir Dushman
NERFINISHED
ⓘ
Owen Willans Richardson NERFINISHED ⓘ |
| predicts |
exponential dependence of emission on work function
ⓘ
quadratic dependence of emission on temperature ⓘ |
| relatedTo |
Child–Langmuir law
NERFINISHED
ⓘ
Fowler–Nordheim equation NERFINISHED ⓘ |
| relates |
thermionic current density to absolute temperature
ⓘ
thermionic current density to work function ⓘ |
| temperatureDependence | strongly temperature dependent ⓘ |
| usedIn |
analysis of hot electron emitters
ⓘ
design of thermionic cathodes ⓘ electron gun design ⓘ vacuum tube engineering ⓘ |
| usesSymbol |
A for Richardson constant
ⓘ
J for current density ⓘ T for absolute temperature ⓘ \phi for work function ⓘ k_B for Boltzmann constant ⓘ |
| validFor | thermionic emission in vacuum ⓘ |
How these facts were elicited
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Subject: Richardson–Dushman equation Description of subject: The Richardson–Dushman equation is a fundamental formula in thermionic emission theory that relates the current density of electrons emitted from a heated metal surface to its temperature and material-specific constants.
Referenced by (1)
Full triples — surface form annotated when it differs from this entity's canonical label.