Work in progress

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  <rdf:Description rdf:about="http://qudt.org/vocab/quantitykind/GibbsEnergy">
    <j.0:hasDimensionVector rdf:resource="http://qudt.org/vocab/dimensionvector/A0E0L2I0M1H0T-2D0"/>
    <rdfs:label xml:lang="sl">Prosta entalpija</rdfs:label>
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    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/E_h"/>
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    <rdfs:label xml:lang="fr">enthalpie libre</rdfs:label>
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    <rdfs:label xml:lang="ja">ギブズエネルギー</rdfs:label>
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    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/MegaTOE"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/KiloV-A_Reactive-HR"/>
    <rdfs:label xml:lang="fa">انرژی آزاد گیبس</rdfs:label>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/KiloV-A-HR"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/KiloEV"/>
    <j.0:latexDefinition rdf:datatype="http://qudt.org/schema/qudt/LatexString">$G = H - T \cdot S$, where $H$ is enthalpy, $T$ is thermodynamic temperature and $S$ is entropy.</j.0:latexDefinition>
    <rdfs:label xml:lang="cs">Gibbsova volná energie</rdfs:label>
    <rdfs:label xml:lang="pl">entalpia swobodna</rdfs:label>
    <rdfs:label xml:lang="en">Gibbs energy</rdfs:label>
    <j.0:symbol>G</j.0:symbol>
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    <rdfs:seeAlso rdf:resource="http://qudt.org/vocab/quantitykind/HelmholtzEnergy"/>
    <j.2:altLabel xml:lang="en">Gibbs function</j.2:altLabel>
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    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/THERM_EC"/>
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    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/CAL_TH"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/THM_US"/>
    <rdfs:label xml:lang="pt">energia livre de Gibbs</rdfs:label>
    <j.2:altLabel xml:lang="ms">fungsi Gibbs</j.2:altLabel>
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    <j.1:description rdf:datatype="http://www.w3.org/1999/02/22-rdf-syntax-ns#HTML">"Gibbs Energy} is one of the potentials are used to measure energy changes in systems as they evolve from an initial state to a final state. The potential used depends on the constraints of the system, such as constant temperature or pressure. \textit{Internal Energy} is the internal energy of the system, \textit{Enthalpy} is the internal energy of the system plus the energy related to pressure-volume work, and Helmholtz and Gibbs free energy are the energies available in a system to do useful work when the temperature and volume or the pressure and temperature are fixed, respectively. The name \textit{Gibbs Free Energy" is also used.</j.1:description>
    <j.2:altLabel xml:lang="de">Gibbs-Energie</j.2:altLabel>
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    <rdfs:label xml:lang="ms">Tenaga Gibbs</rdfs:label>
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    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/FemtoJ"/>
    <rdfs:label xml:lang="tr">Gibbs Serbest Enerjisi</rdfs:label>
    <rdfs:label xml:lang="ar">طاقة غيبس الحرة</rdfs:label>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/CAL_IT"/>
    <j.2:altLabel xml:lang="de">Gibbs-Funktion</j.2:altLabel>
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    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/MegaV-A_Reactive-HR"/>
    <rdfs:label xml:lang="ro">Entalpie liberă</rdfs:label>
    <rdfs:label xml:lang="es">Energía de Gibbs</rdfs:label>
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    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/THM_EEC"/>
    <rdfs:label xml:lang="de">freie Enthalpie</rdfs:label>
    <rdfs:label xml:lang="zh">吉布斯自由能</rdfs:label>
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    <j.0:plainTextDescription>"Gibbs Energy} is one of the potentials are used to measure energy changes in systems as they evolve from an initial state to a final state. The potential used depends on the constraints of the system, such as constant temperature or pressure. \textit{Internal Energy} is the internal energy of the system, \textit{Enthalpy} is the internal energy of the system plus the energy related to pressure-volume work, and Helmholtz and Gibbs free energy are the energies available in a system to do useful work when the temperature and volume or the pressure and temperature are fixed, respectively. The name \textit{Gibbs Free Energy" is also used.</j.0:plainTextDescription>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/TeraW-HR"/>
    <rdfs:label xml:lang="ru">энергия Гиббса</rdfs:label>
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    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/QUAD"/>
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    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/PetaJ"/>
    <rdfs:label xml:lang="it">energia libera di Gibbs</rdfs:label>
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@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/GibbsEnergy>
  rdf:type <http://qudt.org/schema/qudt/QuantityKind> ;
  <http://purl.org/dc/terms/description> "\"Gibbs Energy} is one of the potentials are used to measure energy changes in systems as they evolve from an initial state to a final state. The potential used depends on the constraints of the system, such as constant temperature or pressure. \\textit{Internal Energy} is the internal energy of the system, \\textit{Enthalpy} is the internal energy of the system plus the energy related to pressure-volume work, and Helmholtz and Gibbs free energy are the energies available in a system to do useful work when the temperature and volume or the pressure and temperature are fixed, respectively. The name \\textit{Gibbs Free Energy\" is also used."^^rdf:HTML ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/AttoJ> ;
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  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/CAL_IT> ;
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  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/ERG> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/EV> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/E_h> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/ExaJ> ;
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  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/FemtoJ> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/GigaEV> ;
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  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/J> ;
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  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/KiloCAL> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/KiloEV> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/KiloJ> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/KiloV-A-HR> ;
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  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/MegaTOE> ;
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  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/PicoJ> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/PlanckEnergy> ;
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  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/THERM_EC> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/THERM_US> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/THM_EEC> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/THM_US> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/TOE> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/TeraJ> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/TeraW-HR> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/TonEnergy> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/V-A-HR> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/V-A_Reactive-HR> ;
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  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/W-SEC> ;
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  <http://qudt.org/schema/qudt/isoNormativeReference> "http://www.iso.org/iso/catalogue_detail?csnumber=31890"^^xsd:anyURI ;
  <http://qudt.org/schema/qudt/latexDefinition> "$G = H - T \\cdot S$, where $H$ is enthalpy, $T$ is thermodynamic temperature and $S$ is entropy."^^<http://qudt.org/schema/qudt/LatexString> ;
  <http://qudt.org/schema/qudt/plainTextDescription> "\"Gibbs Energy} is one of the potentials are used to measure energy changes in systems as they evolve from an initial state to a final state. The potential used depends on the constraints of the system, such as constant temperature or pressure. \\textit{Internal Energy} is the internal energy of the system, \\textit{Enthalpy} is the internal energy of the system plus the energy related to pressure-volume work, and Helmholtz and Gibbs free energy are the energies available in a system to do useful work when the temperature and volume or the pressure and temperature are fixed, respectively. The name \\textit{Gibbs Free Energy\" is also used." ;
  <http://qudt.org/schema/qudt/symbol> "G" ;
  rdfs:isDefinedBy <http://qudt.org/2.1/vocab/quantitykind> ;
  rdfs:label "Energía de Gibbs"@es ;
  rdfs:label "Entalpie liberă"@ro ;
  rdfs:label "Gibbs Serbest Enerjisi"@tr ;
  rdfs:label "Gibbs energy"@en ;
  rdfs:label "Gibbsova volná energie"@cs ;
  rdfs:label "Prosta entalpija"@sl ;
  rdfs:label "Tenaga Gibbs"@ms ;
  rdfs:label "energia libera di Gibbs"@it ;
  rdfs:label "energia livre de Gibbs"@pt ;
  rdfs:label "entalpia swobodna"@pl ;
  rdfs:label "enthalpie libre"@fr ;
  rdfs:label "freie Enthalpie"@de ;
  rdfs:label "энергия Гиббса"@ru ;
  rdfs:label "انرژی آزاد گیبس"@fa ;
  rdfs:label "طاقة غيبس الحرة"@ar ;
  rdfs:label "ギブズエネルギー"@ja ;
  rdfs:label "吉布斯自由能"@zh ;
  rdfs:seeAlso <http://qudt.org/vocab/quantitykind/Energy> ;
  rdfs:seeAlso <http://qudt.org/vocab/quantitykind/Enthalpy> ;
  rdfs:seeAlso <http://qudt.org/vocab/quantitykind/HelmholtzEnergy> ;
  rdfs:seeAlso <http://qudt.org/vocab/quantitykind/InternalEnergy> ;
  <http://www.w3.org/2004/02/skos/core#altLabel> "Gibbs function"@en ;
  <http://www.w3.org/2004/02/skos/core#altLabel> "Gibbs-Energie"@de ;
  <http://www.w3.org/2004/02/skos/core#altLabel> "Gibbs-Funktion"@de ;
  <http://www.w3.org/2004/02/skos/core#altLabel> "fungsi Gibbs"@ms ;
  <http://www.w3.org/2004/02/skos/core#broader> <http://qudt.org/vocab/quantitykind/Energy> ;
.

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    ,"description":"\"Gibbs Energy} is one of the potentials are used to measure energy changes in systems as they evolve from an initial state to a final state. The potential used depends on the constraints of the system, such as constant temperature or pressure. \\textit{Internal Energy} is the internal energy of the system, \\textit{Enthalpy} is the internal energy of the system plus the energy related to pressure-volume work, and Helmholtz and Gibbs free energy are the energies available in a system to do useful work when the temperature and volume or the pressure and temperature are fixed, respectively. The name \\textit{Gibbs Free Energy\" is also used." 
    ,"description (plain text)":"\"Gibbs Energy} is one of the potentials are used to measure energy changes in systems as they evolve from an initial state to a final state. The potential used depends on the constraints of the system, such as constant temperature or pressure. \\textit{Internal Energy} is the internal energy of the system, \\textit{Enthalpy} is the internal energy of the system plus the energy related to pressure-volume work, and Helmholtz and Gibbs free energy are the energies available in a system to do useful work when the temperature and volume or the pressure and temperature are fixed, respectively. The name \\textit{Gibbs Free Energy\" is also used." 
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    ,"label":"Entalpie liberă" 
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    ,"label":"Gibbsova volná energie" 
    ,"label":"Prosta entalpija" 
    ,"label":"Tenaga Gibbs" 
    ,"label":"energia libera di Gibbs" 
    ,"label":"energia livre de Gibbs" 
    ,"label":"entalpia swobodna" 
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    ,"label":"freie Enthalpie" 
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    ,"label":"انرژی آزاد گیبس" 
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    ,"label":"ギブズエネルギー" 
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  "latexDefinition" : "$G = H - T \\cdot S$, where $H$ is enthalpy, $T$ is thermodynamic temperature and $S$ is entropy.",
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    "@language" : "sl",
    "@value" : "Prosta entalpija"
  }, {
    "@language" : "fr",
    "@value" : "enthalpie libre"
  }, {
    "@language" : "ja",
    "@value" : "ギブズエネルギー"
  }, {
    "@language" : "fa",
    "@value" : "انرژی آزاد گیبس"
  }, {
    "@language" : "cs",
    "@value" : "Gibbsova volná energie"
  }, {
    "@language" : "pl",
    "@value" : "entalpia swobodna"
  }, {
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    "@value" : "Gibbs energy"
  }, {
    "@language" : "pt",
    "@value" : "energia livre de Gibbs"
  }, {
    "@language" : "ms",
    "@value" : "Tenaga Gibbs"
  }, {
    "@language" : "tr",
    "@value" : "Gibbs Serbest Enerjisi"
  }, {
    "@language" : "ar",
    "@value" : "طاقة غيبس الحرة"
  }, {
    "@language" : "ro",
    "@value" : "Entalpie liberă"
  }, {
    "@language" : "es",
    "@value" : "Energía de Gibbs"
  }, {
    "@language" : "de",
    "@value" : "freie Enthalpie"
  }, {
    "@language" : "zh",
    "@value" : "吉布斯自由能"
  }, {
    "@language" : "ru",
    "@value" : "энергия Гиббса"
  }, {
    "@language" : "it",
    "@value" : "energia libera di Gibbs"
  } ],
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    "@language" : "de",
    "@value" : "Gibbs-Energie"
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