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<rdf:Description rdf:about="http://qudt.org/vocab/quantitykind/ElectromagneticPermeability">
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<j.0:informativeReference rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://en.wikipedia.org/wiki/Permeability_(electromagnetism)</j.0:informativeReference>
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$\textit{Permeability}$ 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:latexSymbol rdf:datatype="http://qudt.org/schema/qudt/LatexString">$\mu$</j.0:latexSymbol>
<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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$\\textit{Permeability}$ 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> ;
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<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> ;
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<http://qudt.org/schema/qudt/latexSymbol> "$\\mu$"^^<http://qudt.org/schema/qudt/LatexString> ;
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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> ;
.
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