quantitykind:GibbsEnergy

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

Type
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.

Properties
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.
qudt:latexDefinition
$G = H - T \cdot S$, where $H$ is enthalpy, $T$ is thermodynamic temperature and $S$ is entropy.
Annotations
skos:altLabel
Gibbs function(en)
Gibbs-Energie(de)
Gibbs-Funktion(de)
fungsi Gibbs(ms)
dcterms: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.
rdfs:label
Energía de Gibbs(es)
Entalpie liberă(ro)
Gibbs Serbest Enerjisi(tr)
Gibbs energy(en)
Gibbsova volná energie(cs)
Prosta entalpija(sl)
Tenaga Gibbs(ms)
energia libera di Gibbs(it)
energia livre de Gibbs(pt)
entalpia swobodna(pl)
enthalpie libre(fr)
freie Enthalpie(de)
энергия Гиббса(ru)
انرژی آزاد گیبس(fa)
طاقة غيبس الحرة(ar)
ギブズエネルギー(ja)
吉布斯自由能(zh)
View as:  CSV

Work in progress

RDF/XML
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    <rdfs:label xml:lang="sl">Prosta entalpija</rdfs:label>
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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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    <rdfs:label xml:lang="fa">انرژی آزاد گیبس</rdfs:label>
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    <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/THM_US"/>
    <rdfs:label xml:lang="pt">energia livre de Gibbs</rdfs:label>
    <j.2:altLabel xml:lang="ms">fungsi Gibbs</j.2:altLabel>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/W-HR"/>
    <rdf:type rdf:resource="http://qudt.org/schema/qudt/QuantityKind"/>
    <rdfs:seeAlso rdf:resource="http://qudt.org/vocab/quantitykind/InternalEnergy"/>
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    <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>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/MegaJ"/>
    <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>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/KiloBTU_TH"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/ERG"/>
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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/PetaJ"/>
    <rdfs:label xml:lang="it">energia libera di Gibbs</rdfs:label>
    <rdfs:seeAlso rdf:resource="http://qudt.org/vocab/quantitykind/Energy"/>
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TURTLE
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@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 ;
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  <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> ;
.
JSON
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 ,"properties":["alternative label":"Gibbs function" 
    ,"alternative label":"Gibbs-Energie" 
    ,"alternative label":"Gibbs-Funktion" 
    ,"alternative label":"fungsi Gibbs" 
    ,"applicable unit":"unit:AttoJ" 
    ,"applicable unit":"unit:BTU_IT" 
    ,"applicable unit":"unit:BTU_TH" 
    ,"applicable unit":"unit:CAL_IT" 
    ,"applicable unit":"unit:CAL_TH" 
    ,"applicable unit":"unit:ERG" 
    ,"applicable unit":"unit:EV" 
    ,"applicable unit":"unit:E_h" 
    ,"applicable unit":"unit:ExaJ" 
    ,"applicable unit":"unit:FT-LB_F" 
    ,"applicable unit":"unit:FT-PDL" 
    ,"applicable unit":"unit:FemtoJ" 
    ,"applicable unit":"unit:GigaEV" 
    ,"applicable unit":"unit:GigaJ" 
    ,"applicable unit":"unit:GigaW-HR" 
    ,"applicable unit":"unit:J" 
    ,"applicable unit":"unit:KiloBTU_IT" 
    ,"applicable unit":"unit:KiloBTU_TH" 
    ,"applicable unit":"unit:KiloCAL" 
    ,"applicable unit":"unit:KiloEV" 
    ,"applicable unit":"unit:KiloJ" 
    ,"applicable unit":"unit:KiloV-A-HR" 
    ,"applicable unit":"unit:KiloV-A_Reactive-HR" 
    ,"applicable unit":"unit:KiloW-HR" 
    ,"applicable unit":"unit:MegaEV" 
    ,"applicable unit":"unit:MegaJ" 
    ,"applicable unit":"unit:MegaTOE" 
    ,"applicable unit":"unit:MegaV-A-HR" 
    ,"applicable unit":"unit:MegaV-A_Reactive-HR" 
    ,"applicable unit":"unit:MegaW-HR" 
    ,"applicable unit":"unit:MicroJ" 
    ,"applicable unit":"unit:MilliJ" 
    ,"applicable unit":"unit:NanoJ" 
    ,"applicable unit":"unit:PetaJ" 
    ,"applicable unit":"unit:PicoJ" 
    ,"applicable unit":"unit:PlanckEnergy" 
    ,"applicable unit":"unit:QUAD" 
    ,"applicable unit":"unit:THERM_EC" 
    ,"applicable unit":"unit:THERM_US" 
    ,"applicable unit":"unit:THM_EEC" 
    ,"applicable unit":"unit:THM_US" 
    ,"applicable unit":"unit:TOE" 
    ,"applicable unit":"unit:TeraJ" 
    ,"applicable unit":"unit:TeraW-HR" 
    ,"applicable unit":"unit:TonEnergy" 
    ,"applicable unit":"unit:V-A-HR" 
    ,"applicable unit":"unit:V-A_Reactive-HR" 
    ,"applicable unit":"unit:W-HR" 
    ,"applicable unit":"unit:W-SEC" 
    ,"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." 
    ,"has broader":"quantitykind:Energy" 
    ,"has dimension vector":"dimension:A0E0L2I0M1H0T-2D0" 
    ,"informative reference":"http:\/\/en.citizendium.org\/wiki\/Thermodynamics" 
    ,"isDefinedBy":"&lt;http:\/\/qudt.org\/2.1\/vocab\/quantitykind&gt;" 
    ,"label":"Energ&iacute;a de Gibbs" 
    ,"label":"Entalpie liberă" 
    ,"label":"Gibbs Serbest Enerjisi" 
    ,"label":"Gibbs energy" 
    ,"label":"Gibbsova voln&aacute; energie" 
    ,"label":"Prosta entalpija" 
    ,"label":"Tenaga Gibbs" 
    ,"label":"energia libera di Gibbs" 
    ,"label":"energia livre de Gibbs" 
    ,"label":"entalpia swobodna" 
    ,"label":"enthalpie libre" 
    ,"label":"freie Enthalpie" 
    ,"label":"энергия Гиббса" 
    ,"label":"انرژی آزاد گیبس" 
    ,"label":"طاقة غيبس الحرة" 
    ,"label":"ギブズエネルギー" 
    ,"label":"吉布斯自由能" 
    ,"latex definition":"$G = H - T \\cdot S$, where $H$ is enthalpy, $T$ is thermodynamic temperature and $S$ is entropy." 
    ,"normative reference (ISO)":"http:\/\/www.iso.org\/iso\/catalogue_detail?csnumber=31890" 
    ,"seeAlso":"quantitykind:Energy" 
    ,"seeAlso":"quantitykind:Enthalpy" 
    ,"seeAlso":"quantitykind:HelmholtzEnergy" 
    ,"seeAlso":"quantitykind:InternalEnergy" 
    ,"symbol":"G" 
    ,"type":"qudt:QuantityKind" 
    ]}
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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.",
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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"
  }, {
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    "@value" : "entalpia swobodna"
  }, {
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    "@value" : "Gibbs energy"
  }, {
    "@language" : "pt",
    "@value" : "energia livre de Gibbs"
  }, {
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    "@value" : "Tenaga Gibbs"
  }, {
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    "@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"
  }, {
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    "@value" : "энергия Гиббса"
  }, {
    "@language" : "it",
    "@value" : "energia libera di Gibbs"
  } ],
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