`quantitykind:ElectricDisplacement`

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

rdf:type: qudt:QuantityKind

Predicate	Object
`rdf:type`	`qudt:QuantityKind`
`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.
`qudt:applicableUnit`	Show 10 values `unit:A-HR-PER-M2` `unit:C-PER-CentiM2` `unit:C-PER-M2` `unit:C-PER-MilliM2` `unit:C_Ab-PER-CentiM2` `unit:C_Stat-PER-CentiM2` `unit:KiloC-PER-M2` `unit:MegaC-PER-M2` `unit:MicroC-PER-M2` `unit:MilliC-PER-M2`
`qudt:exactMatch`	`quantitykind:ElectricFluxDensity`
`qudt:hasDimensionVector`	`qkdv:A0E1L-2I0M0H0T1D0`
`qudt:informativeReference`	http://www.iso.org/iso/home/store/catalogue_tc/catalogue_detail.htm?csnumber=31891 http://www.oxfordreference.com/view/10.1093/acref/9780199233991.001.0001/acref-9780199233991-e-895
`qudt:latexDefinition`	\(D = \epsilon_0 E + P\), where \(\epsilon_0\) is the electric constant, \(E\) is electric field strength, and \(P\) is electric polarization.
`qudt:symbol`	“D”
`rdfs:comment`	“Applicable units are those of quantitykind:ElectricChargePerArea”
`rdfs:isDefinedBy`	http://qudt.org/3.1.10/vocab/quantitykind
`rdfs:label`	“Electric Displacement”@en
`skos:broader`	`quantitykind:ElectricChargePerArea`

Generated 2026-01-15T09:03:10.866-05:00