<rdf:RDF
xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#"
xmlns:j.0="http://qudt.org/schema/qudt/"
xmlns:j.1="http://purl.org/dc/terms/"
xmlns:owl="http://www.w3.org/2002/07/owl#"
xmlns:j.2="http://www.w3.org/2004/02/skos/core#"
xmlns:rdfs="http://www.w3.org/2000/01/rdf-schema#"
xmlns:xsd="http://www.w3.org/2001/XMLSchema#" >
<rdf:Description rdf:about="http://qudt.org/vocab/quantitykind/MutualInductance">
<j.2:broader rdf:resource="http://qudt.org/vocab/quantitykind/Inductance"/>
<rdfs:comment>Applicable units are those of quantitykind:Inductance</rdfs:comment>
<j.1:description rdf:datatype="http://qudt.org/schema/qudt/LatexString">$\textit{Mutual Inductance}$ is the non-diagonal term of the inductance matrix. For two loops, the symbol $M$ is used for $L_{12}$.</j.1:description>
<j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/H_Ab"/>
<j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/MicroH"/>
<j.0:latexDefinition rdf:datatype="http://qudt.org/schema/qudt/LatexString">$L_{mn} = \frac{\Psi_m}{I_n}$, where $I_n$ is an electric current in a thin conducting loop $n$ and $\Psi_m$ is the linked flux caused by that electric current in another loop $m$.</j.0:latexDefinition>
<j.0:informativeReference rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://www.electropedia.org/iev/iev.nsf/display?openform&ievref=131-12-36</j.0:informativeReference>
<rdfs:seeAlso rdf:resource="http://qudt.org/vocab/quantitykind/Inductance"/>
<j.0:hasDimensionVector rdf:resource="http://qudt.org/vocab/dimensionvector/A0E-2L2I0M1H0T-2D0"/>
<j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/MilliH"/>
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<j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/H"/>
<rdf:type rdf:resource="http://qudt.org/schema/qudt/QuantityKind"/>
<j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/KiloH"/>
<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>
<j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/H_Stat"/>
<j.0:symbol>L_{mn}</j.0:symbol>
<j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/NanoH"/>
<j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/PicoH"/>
<rdfs:label xml:lang="en">Mutual Inductance</rdfs:label>
</rdf:Description>
</rdf:RDF>
@prefix owl: <http://www.w3.org/2002/07/owl#> .
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@prefix rdfs: <http://www.w3.org/2000/01/rdf-schema#> .
@prefix xsd: <http://www.w3.org/2001/XMLSchema#> .
<http://qudt.org/vocab/quantitykind/MutualInductance>
rdf:type <http://qudt.org/schema/qudt/QuantityKind> ;
<http://purl.org/dc/terms/description> "$\\textit{Mutual Inductance}$ is the non-diagonal term of the inductance matrix. For two loops, the symbol $M$ is used for $L_{12}$."^^<http://qudt.org/schema/qudt/LatexString> ;
<http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/H> ;
<http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/H_Ab> ;
<http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/H_Stat> ;
<http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/KiloH> ;
<http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/MicroH> ;
<http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/MilliH> ;
<http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/NanoH> ;
<http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/PicoH> ;
<http://qudt.org/schema/qudt/hasDimensionVector> <http://qudt.org/vocab/dimensionvector/A0E-2L2I0M1H0T-2D0> ;
<http://qudt.org/schema/qudt/informativeReference> "http://www.electropedia.org/iev/iev.nsf/display?openform&ievref=131-12-36"^^xsd:anyURI ;
<http://qudt.org/schema/qudt/informativeReference> "http://www.iso.org/iso/home/store/catalogue_tc/catalogue_detail.htm?csnumber=31891"^^xsd:anyURI ;
<http://qudt.org/schema/qudt/latexDefinition> "$L_{mn} = \\frac{\\Psi_m}{I_n}$, where $I_n$ is an electric current in a thin conducting loop $n$ and $\\Psi_m$ is the linked flux caused by that electric current in another loop $m$."^^<http://qudt.org/schema/qudt/LatexString> ;
<http://qudt.org/schema/qudt/symbol> "L_{mn}" ;
rdfs:comment "Applicable units are those of quantitykind:Inductance" ;
rdfs:isDefinedBy <http://qudt.org/2.1/vocab/quantitykind> ;
rdfs:label "Mutual Inductance"@en ;
rdfs:seeAlso <http://qudt.org/vocab/quantitykind/Inductance> ;
<http://www.w3.org/2004/02/skos/core#broader> <http://qudt.org/vocab/quantitykind/Inductance> ;
.
{"resource":"Mutual Inductance"
,"qname":"quantitykind:MutualInductance"
,"uri":"http:\/\/qudt.org\/vocab\/quantitykind\/MutualInductance"
,"properties":["applicable unit":"unit:H"
,"applicable unit":"unit:H_Ab"
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,"applicable unit":"unit:KiloH"
,"applicable unit":"unit:MicroH"
,"applicable unit":"unit:MilliH"
,"applicable unit":"unit:NanoH"
,"applicable unit":"unit:PicoH"
,"comment":"Applicable units are those of quantitykind:Inductance"
,"description":"$\\textit{Mutual Inductance}$ is the non-diagonal term of the inductance matrix. For two loops, the symbol $M$ is used for $L_{12}$."
,"has broader":"quantitykind:Inductance"
,"has dimension vector":"dimension:A0E-2L2I0M1H0T-2D0"
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,"isDefinedBy":"<http:\/\/qudt.org\/2.1\/vocab\/quantitykind>"
,"label":"Mutual Inductance"
,"latex definition":"$L_{mn} = \\frac{\\Psi_m}{I_n}$, where $I_n$ is an electric current in a thin conducting loop $n$ and $\\Psi_m$ is the linked flux caused by that electric current in another loop $m$."
,"seeAlso":"quantitykind:Inductance"
,"symbol":"L_{mn}"
,"type":"qudt:QuantityKind"
]}
{
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"description" : "$\\textit{Mutual Inductance}$ is the non-diagonal term of the inductance matrix. For two loops, the symbol $M$ is used for $L_{12}$.",
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