quantitykind:MagnetomotiveForce

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

Type
Description

$\text{Magnetomotive Force}$, also referred to as ($mmf$), is the ability of an electric circuit to produce magnetic flux. Just as the ability of a battery to produce electric current is called its electromotive force or emf, mmf is taken as the work required to move a unit magnet pole from any point through any path which links the electric circuit back the same point in the presence of the magnetic force produced by the electric current in the circuit. $\text{Magnetomotive Force}$ is the scalar line integral of the magnetic field strength along a closed path.

Properties
qudt:latexDefinition
$F_m = \oint \mathbf{H} \cdot dr$, where $\mathbf{H}$ is magnetic field strength and $r$ is position vector along a given curve $C$ from point $a$ to point $b$.
Annotations
rdfs:comment
Applicable units are those of quantitykind:MagnetomotiveForce
dcterms:description
$\text{Magnetomotive Force}$, also referred to as ($mmf$), is the ability of an electric circuit to produce magnetic flux. Just as the ability of a battery to produce electric current is called its electromotive force or emf, mmf is taken as the work required to move a unit magnet pole from any point through any path which links the electric circuit back the same point in the presence of the magnetic force produced by the electric current in the circuit. $\text{Magnetomotive Force}$ is the scalar line integral of the magnetic field strength along a closed path.
rdfs:label
Magnetomotive Force(en)
View as:  CSV

Work in progress

RDF/XML
<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: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/MagnetomotiveForce">
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/GigaA"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/GI"/>
    <rdf:type rdf:resource="http://qudt.org/schema/qudt/QuantityKind"/>
    <j.0:dbpediaMatch rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://dbpedia.org/resource/Magnetomotive_force</j.0:dbpediaMatch>
    <j.0:hasDimensionVector rdf:resource="http://qudt.org/vocab/dimensionvector/A0E1L0I0M0H0T0D0"/>
    <rdfs:seeAlso rdf:resource="http://qudt.org/vocab/quantitykind/MagneticFieldStrength_H"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/PetaA"/>
    <rdfs:label xml:lang="en">Magnetomotive Force</rdfs:label>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/A"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/FemtoA"/>
    <rdfs:isDefinedBy rdf:resource="http://qudt.org/2.1/vocab/quantitykind"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/AT"/>
    <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:informativeReference rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://www.electropedia.org/iev/iev.nsf/display?openform&amp;ievref=121-11-60</j.0:informativeReference>
    <rdfs:comment>Applicable units are those of quantitykind:MagnetomotiveForce</rdfs:comment>
    <j.1:description rdf:datatype="http://qudt.org/schema/qudt/LatexString">
$\text{Magnetomotive Force}$, also referred to as ($mmf$), is the ability of an electric circuit to produce magnetic flux. 
  Just as the ability of a battery to produce electric current is called its electromotive force 
  or emf, mmf is taken as the work required to move a unit magnet pole from any point through any path 
  which links the electric circuit back the same point in the presence of the magnetic force produced 
  by the electric current in the circuit. 
$\text{Magnetomotive Force}$ is the scalar line integral of the magnetic field strength along a closed path.
  </j.1:description>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/TeraA"/>
    <j.0:latexDefinition rdf:datatype="http://qudt.org/schema/qudt/LatexString">$F_m = \oint \mathbf{H} \cdot dr$, where $\mathbf{H}$ is magnetic field strength and $r$ is position vector along a given curve $C$ from point $a$ to point $b$.</j.0:latexDefinition>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/OERSTED-CentiM"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/AttoA"/>
    <j.0:latexSymbol rdf:datatype="http://qudt.org/schema/qudt/LatexString">$F_m $</j.0:latexSymbol>
  </rdf:Description>
</rdf:RDF>
TURTLE
@prefix owl: <http://www.w3.org/2002/07/owl#> .
@prefix rdf: <http://www.w3.org/1999/02/22-rdf-syntax-ns#> .
@prefix rdfs: <http://www.w3.org/2000/01/rdf-schema#> .
@prefix xsd: <http://www.w3.org/2001/XMLSchema#> .

<http://qudt.org/vocab/quantitykind/MagnetomotiveForce>
  rdf:type <http://qudt.org/schema/qudt/QuantityKind> ;
  <http://purl.org/dc/terms/description> """
$\\text{Magnetomotive Force}$, also referred to as ($mmf$), is the ability of an electric circuit to produce magnetic flux. 
  Just as the ability of a battery to produce electric current is called its electromotive force 
  or emf, mmf is taken as the work required to move a unit magnet pole from any point through any path 
  which links the electric circuit back the same point in the presence of the magnetic force produced 
  by the electric current in the circuit. 
$\\text{Magnetomotive Force}$ is the scalar line integral of the magnetic field strength along a closed path.
  """^^<http://qudt.org/schema/qudt/LatexString> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/A> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/AT> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/AttoA> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/FemtoA> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/GI> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/GigaA> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/OERSTED-CentiM> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/PetaA> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/TeraA> ;
  <http://qudt.org/schema/qudt/dbpediaMatch> "http://dbpedia.org/resource/Magnetomotive_force"^^xsd:anyURI ;
  <http://qudt.org/schema/qudt/hasDimensionVector> <http://qudt.org/vocab/dimensionvector/A0E1L0I0M0H0T0D0> ;
  <http://qudt.org/schema/qudt/informativeReference> "http://www.electropedia.org/iev/iev.nsf/display?openform&ievref=121-11-60"^^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> "$F_m = \\oint \\mathbf{H} \\cdot dr$, where $\\mathbf{H}$ is magnetic field strength and $r$ is position vector along a given curve $C$ from point $a$ to point $b$."^^<http://qudt.org/schema/qudt/LatexString> ;
  <http://qudt.org/schema/qudt/latexSymbol> "$F_m $"^^<http://qudt.org/schema/qudt/LatexString> ;
  rdfs:comment "Applicable units are those of quantitykind:MagnetomotiveForce" ;
  rdfs:isDefinedBy <http://qudt.org/2.1/vocab/quantitykind> ;
  rdfs:label "Magnetomotive Force"@en ;
  rdfs:seeAlso <http://qudt.org/vocab/quantitykind/MagneticFieldStrength_H> ;
.
JSON
{"resource":"Magnetomotive Force" 
 ,"qname":"quantitykind:MagnetomotiveForce" 
 ,"uri":"http:\/\/qudt.org\/vocab\/quantitykind\/MagnetomotiveForce" 
 ,"properties":["applicable unit":"unit:A" 
    ,"applicable unit":"unit:AT" 
    ,"applicable unit":"unit:AttoA" 
    ,"applicable unit":"unit:FemtoA" 
    ,"applicable unit":"unit:GI" 
    ,"applicable unit":"unit:GigaA" 
    ,"applicable unit":"unit:OERSTED-CentiM" 
    ,"applicable unit":"unit:PetaA" 
    ,"applicable unit":"unit:TeraA" 
    ,"comment":"Applicable units are those of quantitykind:MagnetomotiveForce" 
    ,"dbpedia match":"http:\/\/dbpedia.org\/resource\/Magnetomotive_force" 
    ,"description":"\n$\\text{Magnetomotive Force}$, also referred to as ($mmf$), is the ability of an electric circuit to produce magnetic flux. \n  Just as the ability of a battery to produce electric current is called its electromotive force \n  or emf, mmf is taken as the work required to move a unit magnet pole from any point through any path \n  which links the electric circuit back the same point in the presence of the magnetic force produced \n  by the electric current in the circuit. \n$\\text{Magnetomotive Force}$ is the scalar line integral of the magnetic field strength along a closed path.\n  " 
    ,"has dimension vector":"dimension:A0E1L0I0M0H0T0D0" 
    ,"informative reference":"http:\/\/www.electropedia.org\/iev\/iev.nsf\/display?openform&amp;ievref=121-11-60" 
    ,"informative reference":"http:\/\/www.iso.org\/iso\/home\/store\/catalogue_tc\/catalogue_detail.htm?csnumber=31891" 
    ,"isDefinedBy":"&lt;http:\/\/qudt.org\/2.1\/vocab\/quantitykind&gt;" 
    ,"label":"Magnetomotive Force" 
    ,"latex definition":"$F_m = \\oint \\mathbf{H} \\cdot dr$, where $\\mathbf{H}$ is magnetic field strength and $r$ is position vector along a given curve $C$ from point $a$ to point $b$." 
    ,"latex symbol":"$F_m $" 
    ,"seeAlso":"quantitykind:MagneticFieldStrength_H" 
    ,"type":"qudt:QuantityKind" 
    ]}
JSON-LD
{
  "@id" : "http://qudt.org/vocab/quantitykind/MagnetomotiveForce",
  "@type" : "http://qudt.org/schema/qudt/QuantityKind",
  "description" : "\n$\\text{Magnetomotive Force}$, also referred to as ($mmf$), is the ability of an electric circuit to produce magnetic flux. \n  Just as the ability of a battery to produce electric current is called its electromotive force \n  or emf, mmf is taken as the work required to move a unit magnet pole from any point through any path \n  which links the electric circuit back the same point in the presence of the magnetic force produced \n  by the electric current in the circuit. \n$\\text{Magnetomotive Force}$ is the scalar line integral of the magnetic field strength along a closed path.\n  ",
  "applicableUnit" : [ "http://qudt.org/vocab/unit/GigaA", "http://qudt.org/vocab/unit/GI", "http://qudt.org/vocab/unit/PetaA", "http://qudt.org/vocab/unit/A", "http://qudt.org/vocab/unit/FemtoA", "http://qudt.org/vocab/unit/AT", "http://qudt.org/vocab/unit/TeraA", "http://qudt.org/vocab/unit/OERSTED-CentiM", "http://qudt.org/vocab/unit/AttoA" ],
  "dbpediaMatch" : "http://dbpedia.org/resource/Magnetomotive_force",
  "hasDimensionVector" : "http://qudt.org/vocab/dimensionvector/A0E1L0I0M0H0T0D0",
  "informativeReference" : [ "http://www.iso.org/iso/home/store/catalogue_tc/catalogue_detail.htm?csnumber=31891", "http://www.electropedia.org/iev/iev.nsf/display?openform&ievref=121-11-60" ],
  "latexDefinition" : "$F_m = \\oint \\mathbf{H} \\cdot dr$, where $\\mathbf{H}$ is magnetic field strength and $r$ is position vector along a given curve $C$ from point $a$ to point $b$.",
  "latexSymbol" : "$F_m $",
  "comment" : "Applicable units are those of quantitykind:MagnetomotiveForce",
  "isDefinedBy" : "http://qudt.org/2.1/vocab/quantitykind",
  "label" : {
    "@language" : "en",
    "@value" : "Magnetomotive Force"
  },
  "seeAlso" : "http://qudt.org/vocab/quantitykind/MagneticFieldStrength_H",
  "@context" : {
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    "latexSymbol" : {
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    },
    "rdf" : "http://www.w3.org/1999/02/22-rdf-syntax-ns#",
    "owl" : "http://www.w3.org/2002/07/owl#",
    "xsd" : "http://www.w3.org/2001/XMLSchema#",
    "rdfs" : "http://www.w3.org/2000/01/rdf-schema#"
  }
}

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