@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#> .
@prefix owl: <http://www.w3.org/2002/07/owl#> .
@prefix constant: <http://qudt.org/vocab/constant/> .
@prefix dc: <http://purl.org/dc/elements/1.1/> .
@prefix dcterms: <http://purl.org/dc/terms/> .
@prefix prov: <http://www.w3.org/ns/prov#> .
@prefix qkdv: <http://qudt.org/vocab/dimensionvector/> .
@prefix quantitykind: <http://qudt.org/vocab/quantitykind/> .
@prefix qudt: <http://qudt.org/schema/qudt/> .
@prefix si-quantity: <https://si-digital-framework.org/quantities/> .
@prefix skos: <http://www.w3.org/2004/02/skos/core#> .
@prefix unit: <http://qudt.org/vocab/unit/> .
@prefix vaem: <http://www.linkedmodel.org/schema/vaem#> .
@prefix voag: <http://voag.linkedmodel.org/schema/voag#> .

quantitykind:GibbsEnergy
  a qudt:QuantityKind ;
  dcterms:description """
  $\\textit{Internal Energy}$ 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.
  """^^qudt:LatexString ;
  qudt:applicableUnit unit:AttoJ ;
  qudt:applicableUnit unit:BTU_IT ;
  qudt:applicableUnit unit:BTU_TH ;
  qudt:applicableUnit unit:CAL_IT ;
  qudt:applicableUnit unit:CAL_TH ;
  qudt:applicableUnit unit:ERG ;
  qudt:applicableUnit unit:EV ;
  qudt:applicableUnit unit:E_h ;
  qudt:applicableUnit unit:ExaJ ;
  qudt:applicableUnit unit:FT-LB_F ;
  qudt:applicableUnit unit:FT-PDL ;
  qudt:applicableUnit unit:FemtoJ ;
  qudt:applicableUnit unit:GigaEV ;
  qudt:applicableUnit unit:GigaJ ;
  qudt:applicableUnit unit:GigaW-HR ;
  qudt:applicableUnit unit:J ;
  qudt:applicableUnit unit:KiloBTU_IT ;
  qudt:applicableUnit unit:KiloBTU_TH ;
  qudt:applicableUnit unit:KiloCAL ;
  qudt:applicableUnit unit:KiloEV ;
  qudt:applicableUnit unit:KiloJ ;
  qudt:applicableUnit unit:KiloVA-HR ;
  qudt:applicableUnit unit:KiloW-HR ;
  qudt:applicableUnit unit:MegaBTU_IT ;
  qudt:applicableUnit unit:MegaEV ;
  qudt:applicableUnit unit:MegaJ ;
  qudt:applicableUnit unit:MegaTOE ;
  qudt:applicableUnit unit:MegaVA-HR ;
  qudt:applicableUnit unit:MegaW-HR ;
  qudt:applicableUnit unit:MicroJ ;
  qudt:applicableUnit unit:MilliJ ;
  qudt:applicableUnit unit:NanoJ ;
  qudt:applicableUnit unit:PetaJ ;
  qudt:applicableUnit unit:PicoJ ;
  qudt:applicableUnit unit:PlanckEnergy ;
  qudt:applicableUnit unit:QUAD ;
  qudt:applicableUnit unit:THERM_EC ;
  qudt:applicableUnit unit:THERM_US ;
  qudt:applicableUnit unit:THM_EEC ;
  qudt:applicableUnit unit:THM_US ;
  qudt:applicableUnit unit:TOE ;
  qudt:applicableUnit unit:TeraJ ;
  qudt:applicableUnit unit:TeraW-HR ;
  qudt:applicableUnit unit:TonEnergy ;
  qudt:applicableUnit unit:VA-HR ;
  qudt:applicableUnit unit:W-HR ;
  qudt:applicableUnit unit:W-SEC ;
  qudt:hasDimensionVector qkdv:A0E0L2I0M1H0T-2D0 ;
  qudt:informativeReference "http://en.citizendium.org/wiki/Thermodynamics"^^xsd:anyURI ;
  qudt:isoNormativeReference "http://www.iso.org/iso/catalogue_detail?csnumber=31890"^^xsd:anyURI ;
  qudt:latexDefinition "$G = H - T \\cdot S$, where $H$ is enthalpy, $T$ is thermodynamic temperature and $S$ is entropy."^^qudt:LatexString ;
  qudt:plainTextDescription "Gibbs Energy is one of the potentials 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, 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 Gibbs Free Energy is also used." ;
  qudt:symbol "G" ;
  rdfs:comment "Applicable units are those of quantitykind:Energy" ;
  rdfs:isDefinedBy <http://qudt.org/3.2.1/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 quantitykind:Energy ;
  rdfs:seeAlso quantitykind:Enthalpy ;
  rdfs:seeAlso quantitykind:HelmholtzEnergy ;
  rdfs:seeAlso quantitykind:InternalEnergy ;
  skos:altLabel "Gibbs function"@en ;
  skos:altLabel "Gibbs-Energie"@de ;
  skos:altLabel "Gibbs-Funktion"@de ;
  skos:altLabel "fungsi Gibbs"@ms ;
  skos:broader quantitykind:Energy .