quantitykind:ElectromagneticPermeability

URI: http://qudt.org/vocab/quantitykind/ElectromagneticPermeability

Type
Description

"Permeability} is the degree of magnetization of a material that responds linearly to an applied magnetic field. In general permeability is a tensor-valued quantity. The definition given applies to an isotropic medium. For an anisotropic medium permeability is a second order tensor. In electromagnetism, permeability is the measure of the ability of a material to support the formation of a magnetic field within itself. In other words, it is the degree of magnetization that a material obtains in response to an applied magnetic field. Magnetic permeability is typically represented by the Greek letter $\mu$. The term was coined in September, 1885 by Oliver Heaviside. The reciprocal of magnetic permeability is \textit{Magnetic Reluctivity".

Properties
qudt:latexDefinition
$\mu = \frac{B}{H}$, where $B$ is magnetic flux density, and $H$ is magnetic field strength.
Annotations
dcterms:description
"Permeability} is the degree of magnetization of a material that responds linearly to an applied magnetic field. In general permeability is a tensor-valued quantity. The definition given applies to an isotropic medium. For an anisotropic medium permeability is a second order tensor. In electromagnetism, permeability is the measure of the ability of a material to support the formation of a magnetic field within itself. In other words, it is the degree of magnetization that a material obtains in response to an applied magnetic field. Magnetic permeability is typically represented by the Greek letter $\mu$. The term was coined in September, 1885 by Oliver Heaviside. The reciprocal of magnetic permeability is \textit{Magnetic Reluctivity".
rdfs:label
Permeability(en)
View as:  CSV

Work in progress

RDF/XML
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    xmlns:xsd="http://www.w3.org/2001/XMLSchema#" > 
  <rdf:Description rdf:about="http://qudt.org/vocab/quantitykind/ElectromagneticPermeability">
    <rdfs:seeAlso rdf:resource="http://qudt.org/vocab/quantitykind/MagneticFluxDensity"/>
    <rdf:type rdf:resource="http://qudt.org/schema/qudt/QuantityKind"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/MicroH-PER-M"/>
    <j.0:dbpediaMatch rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://dbpedia.org/resource/Permeability</j.0:dbpediaMatch>
    <j.0:informativeReference rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://en.wikipedia.org/wiki/Permeability_(electromagnetism)</j.0:informativeReference>
    <j.1:description rdf:datatype="http://qudt.org/schema/qudt/LatexString">"Permeability} is the degree of magnetization of a material that responds linearly to an applied magnetic field. In general permeability is a tensor-valued quantity. The definition given applies to an isotropic medium. For an anisotropic medium permeability is a second order tensor. In electromagnetism, permeability is the measure of the ability of a material to support the formation of a magnetic field within itself. In other words, it is the degree of magnetization that a material obtains in response to an applied magnetic field. Magnetic permeability is typically represented by the Greek letter $\mu$. The term was coined in September, 1885 by Oliver Heaviside. The reciprocal of magnetic permeability is \textit{Magnetic Reluctivity".</j.1:description>
    <j.0:exactMatch rdf:resource="http://qudt.org/vocab/quantitykind/Permeability"/>
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    <j.0:hasDimensionVector rdf:resource="http://qudt.org/vocab/dimensionvector/A0E-2L1I0M1H0T-2D0"/>
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    <j.0:latexDefinition rdf:datatype="http://qudt.org/schema/qudt/LatexString">$\mu = \frac{B}{H}$,  where $B$ is magnetic flux density,  and $H$ is magnetic field strength.</j.0:latexDefinition>
    <rdfs:seeAlso rdf:resource="http://qudt.org/vocab/constant/ElectromagneticPermeabilityOfVacuum"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/H_Stat-PER-CentiM"/>
    <rdfs:seeAlso rdf:resource="http://qudt.org/vocab/quantitykind/MagneticFieldStrength_H"/>
    <rdfs:label xml:lang="en">Permeability</rdfs:label>
    <j.0:informativeReference rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://www.iso.org/iso/home/store/catalogue_tc/catalogue_detail.htm?csnumber=31891</j.0:informativeReference>
    <rdfs:seeAlso rdf:resource="http://qudt.org/vocab/constant/MagneticConstant"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/NanoH-PER-M"/>
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TURTLE
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  <http://purl.org/dc/terms/description> "\"Permeability} is the degree of magnetization of a material that responds linearly to an applied magnetic field. In general permeability is a tensor-valued quantity. The definition given applies to an isotropic medium. For an anisotropic medium permeability is a second order tensor. In electromagnetism, permeability is the measure of the ability of a material to support the formation of a magnetic field within itself. In other words, it is the degree of magnetization that a material obtains in response to an applied magnetic field. Magnetic permeability is typically represented by the Greek letter $\\mu$. The term was coined in September, 1885 by Oliver Heaviside. The reciprocal of magnetic permeability is \\textit{Magnetic Reluctivity\"."^^<http://qudt.org/schema/qudt/LatexString> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/H-PER-M> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/H_Stat-PER-CentiM> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/MicroH-PER-M> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/NanoH-PER-M> ;
  <http://qudt.org/schema/qudt/dbpediaMatch> "http://dbpedia.org/resource/Permeability"^^xsd:anyURI ;
  <http://qudt.org/schema/qudt/exactMatch> <http://qudt.org/vocab/quantitykind/Permeability> ;
  <http://qudt.org/schema/qudt/hasDimensionVector> <http://qudt.org/vocab/dimensionvector/A0E-2L1I0M1H0T-2D0> ;
  <http://qudt.org/schema/qudt/informativeReference> "http://en.wikipedia.org/wiki/Permeability_(electromagnetism)"^^xsd:anyURI ;
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  <http://qudt.org/schema/qudt/latexDefinition> "$\\mu = \\frac{B}{H}$,  where $B$ is magnetic flux density,  and $H$ is magnetic field strength."^^<http://qudt.org/schema/qudt/LatexString> ;
  <http://qudt.org/schema/qudt/latexSymbol> "$\\mu$"^^<http://qudt.org/schema/qudt/LatexString> ;
  rdfs:isDefinedBy <http://qudt.org/2.1/vocab/quantitykind> ;
  rdfs:label "Permeability"@en ;
  rdfs:seeAlso <http://qudt.org/vocab/constant/ElectromagneticPermeabilityOfVacuum> ;
  rdfs:seeAlso <http://qudt.org/vocab/constant/MagneticConstant> ;
  rdfs:seeAlso <http://qudt.org/vocab/quantitykind/MagneticFieldStrength_H> ;
  rdfs:seeAlso <http://qudt.org/vocab/quantitykind/MagneticFluxDensity> ;
.
JSON
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    ,"seeAlso":"constant:MagneticConstant" 
    ,"seeAlso":"quantitykind:MagneticFieldStrength_H" 
    ,"seeAlso":"quantitykind:MagneticFluxDensity" 
    ,"type":"qudt:QuantityKind" 
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JSON-LD
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  "description" : "\"Permeability} is the degree of magnetization of a material that responds linearly to an applied magnetic field. In general permeability is a tensor-valued quantity. The definition given applies to an isotropic medium. For an anisotropic medium permeability is a second order tensor. In electromagnetism, permeability is the measure of the ability of a material to support the formation of a magnetic field within itself. In other words, it is the degree of magnetization that a material obtains in response to an applied magnetic field. Magnetic permeability is typically represented by the Greek letter $\\mu$. The term was coined in September, 1885 by Oliver Heaviside. The reciprocal of magnetic permeability is \\textit{Magnetic Reluctivity\".",
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