quantitykind:ElectricDisplacement

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

Type
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.

Properties
qudt:latexDefinition
$D = \epsilon_0 E + P$, where $\epsilon_0$ is the electric constant, $E$ is electric field strength, and $P$ is electric polarization.
Annotations
dcterms: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.
rdfs:label
Electric Displacement(en)
View as:  CSV

Work in progress

RDF/XML
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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/ElectricDisplacement">
    <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>
    <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: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"/>
    <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"/>
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    <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"/>
  </rdf:Description>
</rdf:RDF>
TURTLE
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@prefix xsd: <http://www.w3.org/2001/XMLSchema#> .

<http://qudt.org/vocab/quantitykind/ElectricDisplacement>
  rdf:type <http://qudt.org/schema/qudt/QuantityKind> ;
  <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> ;
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  <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> ;
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  <http://qudt.org/schema/qudt/symbol> "D" ;
  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> ;
.
JSON
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    ,"applicable unit":"unit:C-PER-MilliM2" 
    ,"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" 
    ,"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." 
    ,"exact match":"quantitykind:ElectricFluxDensity" 
    ,"has broader":"quantitykind:ElectricChargePerArea" 
    ,"has dimension vector":"dimension:A0E1L-2I0M0H0T1D0" 
    ,"informative reference":"http:\/\/www.iso.org\/iso\/home\/store\/catalogue_tc\/catalogue_detail.htm?csnumber=31891" 
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    ,"isDefinedBy":"&lt;http:\/\/qudt.org\/2.1\/vocab\/quantitykind&gt;" 
    ,"label":"Electric Displacement" 
    ,"latex definition":"$D = \\epsilon_0 E + P$, where $\\epsilon_0$ is the electric constant, $E$ is electric field strength, and $P$ is electric polarization." 
    ,"symbol":"D" 
    ,"type":"qudt:QuantityKind" 
    ]}
JSON-LD
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  "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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  "symbol" : "D",
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  "label" : {
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    "@value" : "Electric Displacement"
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