Work in progress

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    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/C-PER-MilliM2"/>
    <j.0:hasDimensionVector rdf:resource="http://qudt.org/vocab/dimensionvector/A0E1L-2I0M0H0T1D0"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/MicroC-PER-M2"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/MilliC-PER-M2"/>
    <rdfs:label xml:lang="en">Electric Displacement</rdfs:label>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/MegaC-PER-M2"/>
    <j.0:symbol>D</j.0:symbol>
    <rdfs:isDefinedBy rdf:resource="http://qudt.org/2.1/vocab/quantitykind"/>
    <j.0:latexDefinition rdf:datatype="http://qudt.org/schema/qudt/LatexString">$D = \epsilon_0 E + P$, where $\epsilon_0$ is the electric constant, $E$ is electric field strength, and $P$ is electric polarization.</j.0:latexDefinition>
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    <j.0:exactMatch rdf:resource="http://qudt.org/vocab/quantitykind/ElectricFluxDensity"/>
    <j.2:broader rdf:resource="http://qudt.org/vocab/quantitykind/ElectricChargePerArea"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/C_Stat-PER-CentiM2"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/C-PER-CentiM2"/>
    <rdfs:comment>Applicable units are those of quantitykind:ElectricChargePerArea</rdfs:comment>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/A-HR-PER-M2"/>
    <j.1:description rdf:datatype="http://qudt.org/schema/qudt/LatexString">In a dielectric material the presence of an electric field E causes the bound charges in the material (atomic nuclei and their electrons) to slightly separate, inducing a local electric dipole moment. The Electric Displacement Field, $D$, is a vector field that accounts for the effects of free charges within such dielectric materials. This describes also the charge density on an extended surface that could be causing the field.</j.1:description>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/KiloC-PER-M2"/>
    <rdf:type rdf:resource="http://qudt.org/schema/qudt/QuantityKind"/>
    <j.0:informativeReference rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://www.oxfordreference.com/view/10.1093/acref/9780199233991.001.0001/acref-9780199233991-e-895</j.0:informativeReference>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/C_Ab-PER-CentiM2"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/C-PER-M2"/>
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  <http://purl.org/dc/terms/description> "In a dielectric material the presence of an electric field E causes the bound charges in the material (atomic nuclei and their electrons) to slightly separate, inducing a local electric dipole moment. The Electric Displacement Field, $D$, is a vector field that accounts for the effects of free charges within such dielectric materials. This describes also the charge density on an extended surface that could be causing the field."^^<http://qudt.org/schema/qudt/LatexString> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/A-HR-PER-M2> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/C-PER-CentiM2> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/C-PER-M2> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/C-PER-MilliM2> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/C_Ab-PER-CentiM2> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/C_Stat-PER-CentiM2> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/KiloC-PER-M2> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/MegaC-PER-M2> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/MicroC-PER-M2> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/MilliC-PER-M2> ;
  <http://qudt.org/schema/qudt/exactMatch> <http://qudt.org/vocab/quantitykind/ElectricFluxDensity> ;
  <http://qudt.org/schema/qudt/hasDimensionVector> <http://qudt.org/vocab/dimensionvector/A0E1L-2I0M0H0T1D0> ;
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  <http://qudt.org/schema/qudt/latexDefinition> "$D = \\epsilon_0 E + P$, where $\\epsilon_0$ is the electric constant, $E$ is electric field strength, and $P$ is electric polarization."^^<http://qudt.org/schema/qudt/LatexString> ;
  <http://qudt.org/schema/qudt/symbol> "D" ;
  rdfs:comment "Applicable units are those of quantitykind:ElectricChargePerArea" ;
  rdfs:isDefinedBy <http://qudt.org/2.1/vocab/quantitykind> ;
  rdfs:label "Electric Displacement"@en ;
  <http://www.w3.org/2004/02/skos/core#broader> <http://qudt.org/vocab/quantitykind/ElectricChargePerArea> ;
.

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    ,"applicable unit":"unit:C-PER-CentiM2" 
    ,"applicable unit":"unit:C-PER-M2" 
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    ,"applicable unit":"unit:C_Ab-PER-CentiM2" 
    ,"applicable unit":"unit:C_Stat-PER-CentiM2" 
    ,"applicable unit":"unit:KiloC-PER-M2" 
    ,"applicable unit":"unit:MegaC-PER-M2" 
    ,"applicable unit":"unit:MicroC-PER-M2" 
    ,"applicable unit":"unit:MilliC-PER-M2" 
    ,"comment":"Applicable units are those of quantitykind:ElectricChargePerArea" 
    ,"description":"In a dielectric material the presence of an electric field E causes the bound charges in the material (atomic nuclei and their electrons) to slightly separate, inducing a local electric dipole moment. The Electric Displacement Field, $D$, is a vector field that accounts for the effects of free charges within such dielectric materials. This describes also the charge density on an extended surface that could be causing the field." 
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    ,"label":"Electric Displacement" 
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    ,"symbol":"D" 
    ,"type":"qudt:QuantityKind" 
    ]}

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