Work in progress

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    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/"
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    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/ElectricConductivity">
    <rdfs:label xml:lang="es">conductividad eléctrica</rdfs:label>
    <j.0:hasDimensionVector rdf:resource="http://qudt.org/vocab/dimensionvector/A0E2L-3I0M-1H0T3D0"/>
    <rdfs:label xml:lang="pt">condutividade elétrica</rdfs:label>
    <rdf:type rdf:resource="http://qudt.org/schema/qudt/QuantityKind"/>
    <rdfs:isDefinedBy rdf:resource="http://qudt.org/2.1/vocab/quantitykind"/>
    <rdfs:label xml:lang="fa">رسانايى الکتريکى/هدایت الکتریکی</rdfs:label>
    <j.1:description rdf:datatype="http://qudt.org/schema/qudt/LatexString">
  The quantity kind $\textit{Electric Conductivity}$ or $\textit{Specific Conductance}$ is a measure of a material's ability to conduct an electric current. 
  When an electrical potential difference is placed across a conductor, its movable charges flow, giving rise to an electric current. 
  The conductivity $\sigma$ is defined as the ratio of the electric current density $J$ to the electric field, $E$: $J = \sigma E$. 
  In isotropic materials, conductivity is scalar-valued, however in general, conductivity is a tensor-valued quantity.
  </j.1:description>
    <rdfs:label xml:lang="it">conducibilità elettrica</rdfs:label>
    <rdfs:label xml:lang="fr">conductivité électrique</rdfs:label>
    <j.0:latexSymbol rdf:datatype="http://qudt.org/schema/qudt/LatexString">$\sigma$</j.0:latexSymbol>
    <rdfs:comment>Applicable units are those of quantitykind:ElectricConductivity</rdfs:comment>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/MHO_Stat"/>
    <rdfs:label xml:lang="en">electric conductivity</rdfs:label>
    <rdfs:label xml:lang="tr">elektrik iletkenliği</rdfs:label>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/S_Ab"/>
    <rdfs:label xml:lang="zh">电导率</rdfs:label>
    <rdfs:label xml:lang="ms">Kekonduksian elektrik</rdfs:label>
    <rdfs:label xml:lang="de">elektrische Leitfähigkeit</rdfs:label>
    <rdfs:label xml:lang="sl">električna prevodnost</rdfs:label>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/S_Stat"/>
  </rdf:Description>
</rdf:RDF>

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@prefix xsd: <http://www.w3.org/2001/XMLSchema#> .

<http://qudt.org/vocab/quantitykind/ElectricConductivity>
  rdf:type <http://qudt.org/schema/qudt/QuantityKind> ;
  <http://purl.org/dc/terms/description> """
  The quantity kind $\\textit{Electric Conductivity}$ or $\\textit{Specific Conductance}$ is a measure of a material's ability to conduct an electric current. 
  When an electrical potential difference is placed across a conductor, its movable charges flow, giving rise to an electric current. 
  The conductivity $\\sigma$ is defined as the ratio of the electric current density $J$ to the electric field, $E$: $J = \\sigma E$. 
  In isotropic materials, conductivity is scalar-valued, however in general, conductivity is a tensor-valued quantity.
  """^^<http://qudt.org/schema/qudt/LatexString> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/MHO_Stat> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/S_Ab> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/S_Stat> ;
  <http://qudt.org/schema/qudt/hasDimensionVector> <http://qudt.org/vocab/dimensionvector/A0E2L-3I0M-1H0T3D0> ;
  <http://qudt.org/schema/qudt/latexSymbol> "$\\sigma$"^^<http://qudt.org/schema/qudt/LatexString> ;
  rdfs:comment "Applicable units are those of quantitykind:ElectricConductivity" ;
  rdfs:isDefinedBy <http://qudt.org/2.1/vocab/quantitykind> ;
  rdfs:label "Kekonduksian elektrik"@ms ;
  rdfs:label "conducibilità elettrica"@it ;
  rdfs:label "conductividad eléctrica"@es ;
  rdfs:label "conductivité électrique"@fr ;
  rdfs:label "condutividade elétrica"@pt ;
  rdfs:label "electric conductivity"@en ;
  rdfs:label "elektrik iletkenliği"@tr ;
  rdfs:label "elektrische Leitfähigkeit"@de ;
  rdfs:label "električna prevodnost"@sl ;
  rdfs:label "رسانايى الکتريکى/هدایت الکتریکی"@fa ;
  rdfs:label "电导率"@zh ;
.

{"resource":"electric conductivity" 
 ,"qname":"quantitykind:ElectricConductivity" 
 ,"uri":"http:\/\/qudt.org\/vocab\/quantitykind\/ElectricConductivity" 
 ,"properties":["applicable unit":"unit:MHO_Stat" 
    ,"applicable unit":"unit:S_Ab" 
    ,"applicable unit":"unit:S_Stat" 
    ,"comment":"Applicable units are those of quantitykind:ElectricConductivity" 
    ,"description":"\n  The quantity kind $\\textit{Electric Conductivity}$ or $\\textit{Specific Conductance}$ is a measure of a material's ability to conduct an electric current. \n  When an electrical potential difference is placed across a conductor, its movable charges flow, giving rise to an electric current. \n  The conductivity $\\sigma$ is defined as the ratio of the electric current density $J$ to the electric field, $E$: $J = \\sigma E$. \n  In isotropic materials, conductivity is scalar-valued, however in general, conductivity is a tensor-valued quantity.\n  " 
    ,"has dimension vector":"dimension:A0E2L-3I0M-1H0T3D0" 
    ,"isDefinedBy":"<http:\/\/qudt.org\/2.1\/vocab\/quantitykind>" 
    ,"label":"Kekonduksian elektrik" 
    ,"label":"conducibilità elettrica" 
    ,"label":"conductividad eléctrica" 
    ,"label":"conductivité électrique" 
    ,"label":"condutividade elétrica" 
    ,"label":"electric conductivity" 
    ,"label":"elektrik iletkenliği" 
    ,"label":"elektrische Leitfähigkeit" 
    ,"label":"električna prevodnost" 
    ,"label":"رسانايى الکتريکى\/هدایت الکتریکی" 
    ,"label":"电导率" 
    ,"latex symbol":"$\\sigma$" 
    ,"type":"qudt:QuantityKind" 
    ]}

{
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  "@type" : "http://qudt.org/schema/qudt/QuantityKind",
  "description" : "\n  The quantity kind $\\textit{Electric Conductivity}$ or $\\textit{Specific Conductance}$ is a measure of a material's ability to conduct an electric current. \n  When an electrical potential difference is placed across a conductor, its movable charges flow, giving rise to an electric current. \n  The conductivity $\\sigma$ is defined as the ratio of the electric current density $J$ to the electric field, $E$: $J = \\sigma E$. \n  In isotropic materials, conductivity is scalar-valued, however in general, conductivity is a tensor-valued quantity.\n  ",
  "applicableUnit" : [ "http://qudt.org/vocab/unit/MHO_Stat", "http://qudt.org/vocab/unit/S_Ab", "http://qudt.org/vocab/unit/S_Stat" ],
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  "latexSymbol" : "$\\sigma$",
  "comment" : "Applicable units are those of quantitykind:ElectricConductivity",
  "isDefinedBy" : "http://qudt.org/2.1/vocab/quantitykind",
  "label" : [ {
    "@language" : "es",
    "@value" : "conductividad eléctrica"
  }, {
    "@language" : "pt",
    "@value" : "condutividade elétrica"
  }, {
    "@language" : "fa",
    "@value" : "رسانايى الکتريکى/هدایت الکتریکی"
  }, {
    "@language" : "it",
    "@value" : "conducibilità elettrica"
  }, {
    "@language" : "fr",
    "@value" : "conductivité électrique"
  }, {
    "@language" : "en",
    "@value" : "electric conductivity"
  }, {
    "@language" : "tr",
    "@value" : "elektrik iletkenliği"
  }, {
    "@language" : "zh",
    "@value" : "电导率"
  }, {
    "@language" : "ms",
    "@value" : "Kekonduksian elektrik"
  }, {
    "@language" : "de",
    "@value" : "elektrische Leitfähigkeit"
  }, {
    "@language" : "sl",
    "@value" : "električna prevodnost"
  } ],
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