<rdf:RDF
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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/PoyntingVector">
<j.0:latexSymbol rdf:datatype="http://qudt.org/schema/qudt/LatexString">$\mathbf{S} $</j.0:latexSymbol>
<j.0:informativeReference rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://www.iso.org/iso/home/store/catalogue_tc/catalogue_detail.htm?csnumber=31891</j.0:informativeReference>
<rdfs:label xml:lang="de">Poynting-Vektor</rdfs:label>
<j.0:informativeReference rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://www.electropedia.org/iev/iev.nsf/display?openform&ievref=121-11-66</j.0:informativeReference>
<rdfs:comment>Applicable units are those of quantitykind:PoyntingVector</rdfs:comment>
<rdfs:label xml:lang="ja">ポインティングベクトル</rdfs:label>
<rdfs:isDefinedBy rdf:resource="http://qudt.org/2.1/vocab/quantitykind"/>
<j.0:latexDefinition rdf:datatype="http://qudt.org/schema/qudt/LatexString">$\mathbf{S} = \mathbf{E} \times \mathbf{H} $, where $\mathbf{E}$ is electric field strength and \mathbf{H} is magnetic field strength.</j.0:latexDefinition>
<rdfs:label xml:lang="ru">вектор Пойнтинга</rdfs:label>
<j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/W-PER-M2"/>
<j.1:description rdf:datatype="http://qudt.org/schema/qudt/LatexString">
A $\textit{Poynting Vector}$ is the vector product of the electric field strength $\mathbf{E}$
and the magnetic field strength $\mathbf{H}$ of the electromagnetic field at a given point.
The flux of the Poynting vector through a closed surface is equal to the electromagnetic power passing
through this surface.
For a periodic electromagnetic field, the time average of the Poynting vector is a vector of which,
with certain reservations, the direction may be considered as being the direction of propagation
of electromagnetic energy and the magnitude considered as being the average electromagnetic power
flux density.
</j.1:description>
<rdfs:label xml:lang="it">vettore di Poynting</rdfs:label>
<rdfs:label xml:lang="fr">vecteur de Poynting</rdfs:label>
<rdfs:label xml:lang="en">Poynting vector</rdfs:label>
<rdfs:label xml:lang="ar">متجَه بوينتنج</rdfs:label>
<j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/NanoW-PER-M2"/>
<j.0:plainTextDescription>"Poynting Vector" is the vector product of the electric field strength $\mathbf{E}$ and the magnetic field strength $\mathbf{H}" of the electromagnetic field at a given point. The flux of the Poynting vector through a closed surface is equal to the electromagnetic power passing through this surface. For a periodic electromagnetic field, the time average of the Poynting vector is a vector of which, with certain reservations, the direction may be considered as being the direction of propagation of electromagnetic energy and the magnitude considered as being the average electromagnetic power flux density.</j.0:plainTextDescription>
<rdf:type rdf:resource="http://qudt.org/schema/qudt/QuantityKind"/>
<j.0:expression rdf:datatype="http://qudt.org/schema/qudt/LatexString">$poynting-vector$</j.0:expression>
<rdfs:label xml:lang="pl">wektor Poyntinga</rdfs:label>
<j.0:hasDimensionVector rdf:resource="http://qudt.org/vocab/dimensionvector/A0E0L0I0M1H0T-3D0"/>
<rdfs:label xml:lang="es">vector de Poynting</rdfs:label>
<rdfs:label xml:lang="pt">vector de Poynting</rdfs:label>
</rdf:Description>
</rdf:RDF>
@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/PoyntingVector>
rdf:type <http://qudt.org/schema/qudt/QuantityKind> ;
<http://purl.org/dc/terms/description> """
A $\\textit{Poynting Vector}$ is the vector product of the electric field strength $\\mathbf{E}$
and the magnetic field strength $\\mathbf{H}$ of the electromagnetic field at a given point.
The flux of the Poynting vector through a closed surface is equal to the electromagnetic power passing
through this surface.
For a periodic electromagnetic field, the time average of the Poynting vector is a vector of which,
with certain reservations, the direction may be considered as being the direction of propagation
of electromagnetic energy and the magnitude considered as being the average electromagnetic power
flux density.
"""^^<http://qudt.org/schema/qudt/LatexString> ;
<http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/NanoW-PER-M2> ;
<http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/W-PER-M2> ;
<http://qudt.org/schema/qudt/expression> "$poynting-vector$"^^<http://qudt.org/schema/qudt/LatexString> ;
<http://qudt.org/schema/qudt/hasDimensionVector> <http://qudt.org/vocab/dimensionvector/A0E0L0I0M1H0T-3D0> ;
<http://qudt.org/schema/qudt/informativeReference> "http://www.electropedia.org/iev/iev.nsf/display?openform&ievref=121-11-66"^^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> "$\\mathbf{S} = \\mathbf{E} \\times \\mathbf{H} $, where $\\mathbf{E}$ is electric field strength and \\mathbf{H} is magnetic field strength."^^<http://qudt.org/schema/qudt/LatexString> ;
<http://qudt.org/schema/qudt/latexSymbol> "$\\mathbf{S} $"^^<http://qudt.org/schema/qudt/LatexString> ;
<http://qudt.org/schema/qudt/plainTextDescription> "\"Poynting Vector\" is the vector product of the electric field strength $\\mathbf{E}$ and the magnetic field strength $\\mathbf{H}\" of the electromagnetic field at a given point. The flux of the Poynting vector through a closed surface is equal to the electromagnetic power passing through this surface. For a periodic electromagnetic field, the time average of the Poynting vector is a vector of which, with certain reservations, the direction may be considered as being the direction of propagation of electromagnetic energy and the magnitude considered as being the average electromagnetic power flux density." ;
rdfs:comment "Applicable units are those of quantitykind:PoyntingVector" ;
rdfs:isDefinedBy <http://qudt.org/2.1/vocab/quantitykind> ;
rdfs:label "Poynting vector"@en ;
rdfs:label "Poynting-Vektor"@de ;
rdfs:label "vecteur de Poynting"@fr ;
rdfs:label "vector de Poynting"@es ;
rdfs:label "vector de Poynting"@pt ;
rdfs:label "vettore di Poynting"@it ;
rdfs:label "wektor Poyntinga"@pl ;
rdfs:label "вектор Пойнтинга"@ru ;
rdfs:label "متجَه بوينتنج"@ar ;
rdfs:label "ポインティングベクトル"@ja ;
.
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,"description (plain text)":"\"Poynting Vector\" is the vector product of the electric field strength $\\mathbf{E}$ and the magnetic field strength $\\mathbf{H}\" of the electromagnetic field at a given point. The flux of the Poynting vector through a closed surface is equal to the electromagnetic power passing through this surface. For a periodic electromagnetic field, the time average of the Poynting vector is a vector of which, with certain reservations, the direction may be considered as being the direction of propagation of electromagnetic energy and the magnitude considered as being the average electromagnetic power flux density."
,"expression":"$poynting-vector$"
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,"isDefinedBy":"<http:\/\/qudt.org\/2.1\/vocab\/quantitykind>"
,"label":"Poynting vector"
,"label":"Poynting-Vektor"
,"label":"vecteur de Poynting"
,"label":"vector de Poynting"
,"label":"vector de Poynting"
,"label":"vettore di Poynting"
,"label":"wektor Poyntinga"
,"label":"вектор Пойнтинга"
,"label":"متجَه بوينتنج"
,"label":"ポインティングベクトル"
,"latex definition":"$\\mathbf{S} = \\mathbf{E} \\times \\mathbf{H} $, where $\\mathbf{E}$ is electric field strength and \\mathbf{H} is magnetic field strength."
,"latex symbol":"$\\mathbf{S} $"
,"type":"qudt:QuantityKind"
]}
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"description" : "\n A $\\textit{Poynting Vector}$ is the vector product of the electric field strength $\\mathbf{E}$\n and the magnetic field strength $\\mathbf{H}$ of the electromagnetic field at a given point. \n The flux of the Poynting vector through a closed surface is equal to the electromagnetic power passing\n through this surface. \n For a periodic electromagnetic field, the time average of the Poynting vector is a vector of which,\n with certain reservations, the direction may be considered as being the direction of propagation\n of electromagnetic energy and the magnitude considered as being the average electromagnetic power\n flux density.\n ",
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"comment" : "Applicable units are those of quantitykind:PoyntingVector",
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"label" : [ {
"@language" : "de",
"@value" : "Poynting-Vektor"
}, {
"@language" : "ja",
"@value" : "ポインティングベクトル"
}, {
"@language" : "ru",
"@value" : "вектор Пойнтинга"
}, {
"@language" : "it",
"@value" : "vettore di Poynting"
}, {
"@language" : "fr",
"@value" : "vecteur de Poynting"
}, {
"@language" : "en",
"@value" : "Poynting vector"
}, {
"@language" : "ar",
"@value" : "متجَه بوينتنج"
}, {
"@language" : "pl",
"@value" : "wektor Poyntinga"
}, {
"@language" : "es",
"@value" : "vector de Poynting"
}, {
"@language" : "pt",
"@value" : "vector de Poynting"
} ],
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