quantitykind:Work

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

Type
Description

$\textit{Work}$ or $net\ work$ is equal to the change in kinetic energy. This relationship is called the work-energy theorem: $$Wnet = K. E._f K. E._o $$ where $K. E._f$ is the final kinetic energy and $K. E._o$ is the original kinetic energy. Potential energy, also referred to as stored energy, is the ability of a system to do work due to its position or internal structure. Change in potential energy is equal to work. The potential energy equations can also be derived from the integral form of work: $$\Delta P. E. = W = \int F \cdot dx$$.

Properties
qudt:applicableUnit
qudt:plainTextDescription
A force is said to do Work when it acts on a body so that there is a displacement of the point of application, however small, in the direction of the force. The concepts of work and energy are closely tied to the concept of force because an applied force can do work on an object and cause a change in energy. Energy is defined as the ability to do work. Work is done on an object when an applied force moves it through a distance. Kinetic energy is the energy of an object in motion. The net work is equal to the change in kinetic energy.
skos:broader
qudt:hasDimensionVector
qudt:latexDefinition
$A = \int Pdt$, where $P$ is power and $t$ is time.
qudt:isoNormativeReference
qudt:symbol
A
rdf:type
Annotations
rdfs:comment
Applicable units are those of quantitykind:Energy
dcterms:description
$\textit{Work}$ or $net\ work$ is equal to the change in kinetic energy. This relationship is called the work-energy theorem: $$Wnet = K. E._f K. E._o $$ where $K. E._f$ is the final kinetic energy and $K. E._o$ is the original kinetic energy. Potential energy, also referred to as stored energy, is the ability of a system to do work due to its position or internal structure. Change in potential energy is equal to work. The potential energy equations can also be derived from the integral form of work: $$\Delta P. E. = W = \int F \cdot dx$$.
qudt:informativeReference
rdfs:isDefinedBy
rdfs:label
Arbeit(de)
delo(sl)
iş(tr)
kerja(ms)
lavoro(it)
lucru mecanic(ro)
praca(pl)
práce(cs)
trabajo(es)
trabalho(pt)
travail(fr)
work(en)
کار(fa)
कार्य(hi)
仕事量(ja)
功(zh)
View as:  CSV

Work in progress

RDF/XML 
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  $\textit{Work}$ or $net\ work$ is equal to the change in kinetic energy. 
  This relationship is called the work-energy theorem: 
  $$Wnet = K. E._f  K. E._o $$
   where $K. E._f$ is the final kinetic energy and $K. E._o$ is the original kinetic energy. 
  Potential energy, also referred to as stored energy, is the ability of a system to do work due to its position or internal structure. 
  Change in potential energy is equal to work. 
  The potential energy equations can also be derived from the integral form of work:
  $$\Delta P. E. = W = \int  F \cdot dx$$.
  </j.1:description>
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    <j.0:plainTextDescription>A force is said to do Work when it acts on a body so that there is a displacement of the point of application, however small, in the direction of the force.  The concepts of work and energy are closely tied to the concept of force because an applied force can do work on an object and cause a change in energy. Energy is defined as the ability to do work. Work is done on an object when an applied force moves it through a distance. Kinetic energy is the energy of an object in motion. The net work is equal to the change in kinetic energy.</j.0:plainTextDescription>
    <rdfs:label xml:lang="ja">仕事量</rdfs:label>
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    <rdfs:label xml:lang="zh">功</rdfs:label>
    <rdfs:label xml:lang="tr">iş</rdfs:label>
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TURTLE 
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<http://qudt.org/vocab/quantitykind/Work>
  rdf:type <http://qudt.org/schema/qudt/QuantityKind> ;
  <http://purl.org/dc/terms/description> """
  $\\textit{Work}$ or $net\\ work$ is equal to the change in kinetic energy. 
  This relationship is called the work-energy theorem: 
  $$Wnet = K. E._f  K. E._o $$
   where $K. E._f$ is the final kinetic energy and $K. E._o$ is the original kinetic energy. 
  Potential energy, also referred to as stored energy, is the ability of a system to do work due to its position or internal structure. 
  Change in potential energy is equal to work. 
  The potential energy equations can also be derived from the integral form of work:
  $$\\Delta P. E. = W = \\int  F \\cdot dx$$.
  """^^<http://qudt.org/schema/qudt/LatexString> ;
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  <http://qudt.org/schema/qudt/symbol> "A" ;
  rdfs:comment "Applicable units are those of quantitykind:Energy" ;
  rdfs:isDefinedBy <http://qudt.org/2.1/vocab/quantitykind> ;
  rdfs:label "Arbeit"@de ;
  rdfs:label "delo"@sl ;
  rdfs:label "iş"@tr ;
  rdfs:label "kerja"@ms ;
  rdfs:label "lavoro"@it ;
  rdfs:label "lucru mecanic"@ro ;
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  rdfs:label "práce"@cs ;
  rdfs:label "trabajo"@es ;
  rdfs:label "trabalho"@pt ;
  rdfs:label "travail"@fr ;
  rdfs:label "work"@en ;
  rdfs:label "کار"@fa ;
  rdfs:label "कार्य"@hi ;
  rdfs:label "仕事量"@ja ;
  rdfs:label "功"@zh ;
  <http://www.w3.org/2004/02/skos/core#broader> <http://qudt.org/vocab/quantitykind/Energy> ;
.
JSON 
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    ,"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" 
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    ,"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" 
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    ,"applicable unit":"unit:W-HR" 
    ,"applicable unit":"unit:W-SEC" 
    ,"comment":"Applicable units are those of quantitykind:Energy" 
    ,"description":"\n  $\\textit{Work}$ or $net\\ work$ is equal to the change in kinetic energy. \n  This relationship is called the work-energy theorem: \n  $$Wnet = K. E._f  K. E._o $$\n   where $K. E._f$ is the final kinetic energy and $K. E._o$ is the original kinetic energy. \n  Potential energy, also referred to as stored energy, is the ability of a system to do work due to its position or internal structure. \n  Change in potential energy is equal to work. \n  The potential energy equations can also be derived from the integral form of work:\n  $$\\Delta P. E. = W = \\int  F \\cdot dx$$.\n  " 
    ,"description (plain text)":"A force is said to do Work when it acts on a body so that there is a displacement of the point of application, however small, in the direction of the force.  The concepts of work and energy are closely tied to the concept of force because an applied force can do work on an object and cause a change in energy. Energy is defined as the ability to do work. Work is done on an object when an applied force moves it through a distance. Kinetic energy is the energy of an object in motion. The net work is equal to the change in kinetic energy." 
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    ,"label":"Arbeit" 
    ,"label":"delo" 
    ,"label":"iş" 
    ,"label":"kerja" 
    ,"label":"lavoro" 
    ,"label":"lucru mecanic" 
    ,"label":"praca" 
    ,"label":"pr&aacute;ce" 
    ,"label":"trabajo" 
    ,"label":"trabalho" 
    ,"label":"travail" 
    ,"label":"work" 
    ,"label":"کار" 
    ,"label":"कार्य" 
    ,"label":"仕事量" 
    ,"label":"功" 
    ,"latex definition":"$A = \\int Pdt$, where $P$ is power and $t$ is time." 
    ,"normative reference (ISO)":"http:\/\/www.iso.org\/iso\/catalogue_detail?csnumber=31889" 
    ,"symbol":"A" 
    ,"type":"qudt:QuantityKind" 
    ]}
JSON-LD 
{
  "@id" : "http://qudt.org/vocab/quantitykind/Work",
  "@type" : "http://qudt.org/schema/qudt/QuantityKind",
  "description" : "\n  $\\textit{Work}$ or $net\\ work$ is equal to the change in kinetic energy. \n  This relationship is called the work-energy theorem: \n  $$Wnet = K. E._f  K. E._o $$\n   where $K. E._f$ is the final kinetic energy and $K. E._o$ is the original kinetic energy. \n  Potential energy, also referred to as stored energy, is the ability of a system to do work due to its position or internal structure. \n  Change in potential energy is equal to work. \n  The potential energy equations can also be derived from the integral form of work:\n  $$\\Delta P. E. = W = \\int  F \\cdot dx$$.\n  ",
  "applicableUnit" : [ "http://qudt.org/vocab/unit/THM_US", "http://qudt.org/vocab/unit/V-A_Reactive-HR", "http://qudt.org/vocab/unit/ERG", "http://qudt.org/vocab/unit/MicroJ", "http://qudt.org/vocab/unit/MegaJ", "http://qudt.org/vocab/unit/PlanckEnergy", "http://qudt.org/vocab/unit/CAL_TH", "http://qudt.org/vocab/unit/MegaV-A_Reactive-HR", "http://qudt.org/vocab/unit/MegaW-HR", "http://qudt.org/vocab/unit/KiloCAL", "http://qudt.org/vocab/unit/BTU_IT", "http://qudt.org/vocab/unit/TonEnergy", "http://qudt.org/vocab/unit/GigaW-HR", "http://qudt.org/vocab/unit/PetaJ", "http://qudt.org/vocab/unit/E_h", "http://qudt.org/vocab/unit/GigaJ", "http://qudt.org/vocab/unit/GigaEV", "http://qudt.org/vocab/unit/THERM_EC", "http://qudt.org/vocab/unit/W-SEC", "http://qudt.org/vocab/unit/PicoJ", "http://qudt.org/vocab/unit/FemtoJ", "http://qudt.org/vocab/unit/MegaTOE", "http://qudt.org/vocab/unit/J", "http://qudt.org/vocab/unit/KiloBTU_IT", "http://qudt.org/vocab/unit/FT-LB_F", "http://qudt.org/vocab/unit/KiloBTU_TH", "http://qudt.org/vocab/unit/TeraJ", "http://qudt.org/vocab/unit/MegaEV", "http://qudt.org/vocab/unit/THERM_US", "http://qudt.org/vocab/unit/KiloV-A_Reactive-HR", "http://qudt.org/vocab/unit/W-HR", "http://qudt.org/vocab/unit/FT-PDL", "http://qudt.org/vocab/unit/MegaV-A-HR", "http://qudt.org/vocab/unit/V-A-HR", "http://qudt.org/vocab/unit/EV", "http://qudt.org/vocab/unit/THM_EEC", "http://qudt.org/vocab/unit/QUAD", "http://qudt.org/vocab/unit/KiloV-A-HR", "http://qudt.org/vocab/unit/ExaJ", "http://qudt.org/vocab/unit/KiloW-HR", "http://qudt.org/vocab/unit/KiloJ", "http://qudt.org/vocab/unit/CAL_IT", "http://qudt.org/vocab/unit/NanoJ", "http://qudt.org/vocab/unit/TOE", "http://qudt.org/vocab/unit/BTU_TH", "http://qudt.org/vocab/unit/AttoJ", "http://qudt.org/vocab/unit/KiloEV", "http://qudt.org/vocab/unit/TeraW-HR", "http://qudt.org/vocab/unit/MilliJ" ],
  "hasDimensionVector" : "http://qudt.org/vocab/dimensionvector/A0E0L2I0M1H0T-2D0",
  "informativeReference" : [ "http://www.cliffsnotes.com/study_guide/Work-and-Energy.topicArticleId-10453,articleId-10418.html", "http://en.wikipedia.org/wiki/Work_(physics)" ],
  "isoNormativeReference" : "http://www.iso.org/iso/catalogue_detail?csnumber=31889",
  "latexDefinition" : "$A = \\int Pdt$, where $P$ is power and $t$ is time.",
  "plainTextDescription" : "A force is said to do Work when it acts on a body so that there is a displacement of the point of application, however small, in the direction of the force.  The concepts of work and energy are closely tied to the concept of force because an applied force can do work on an object and cause a change in energy. Energy is defined as the ability to do work. Work is done on an object when an applied force moves it through a distance. Kinetic energy is the energy of an object in motion. The net work is equal to the change in kinetic energy.",
  "symbol" : "A",
  "comment" : "Applicable units are those of quantitykind:Energy",
  "isDefinedBy" : "http://qudt.org/2.1/vocab/quantitykind",
  "label" : [ {
    "@language" : "fr",
    "@value" : "travail"
  }, {
    "@language" : "pl",
    "@value" : "praca"
  }, {
    "@language" : "cs",
    "@value" : "práce"
  }, {
    "@language" : "de",
    "@value" : "Arbeit"
  }, {
    "@language" : "sl",
    "@value" : "delo"
  }, {
    "@language" : "pt",
    "@value" : "trabalho"
  }, {
    "@language" : "ro",
    "@value" : "lucru mecanic"
  }, {
    "@language" : "ja",
    "@value" : "仕事量"
  }, {
    "@language" : "hi",
    "@value" : "कार्य"
  }, {
    "@language" : "ms",
    "@value" : "kerja"
  }, {
    "@language" : "zh",
    "@value" : "功"
  }, {
    "@language" : "tr",
    "@value" : "iş"
  }, {
    "@language" : "en",
    "@value" : "work"
  }, {
    "@language" : "fa",
    "@value" : "کار"
  }, {
    "@language" : "es",
    "@value" : "trabajo"
  }, {
    "@language" : "it",
    "@value" : "lavoro"
  } ],
  "broader" : "http://qudt.org/vocab/quantitykind/Energy",
  "@context" : {
    "applicableUnit" : {
      "@id" : "http://qudt.org/schema/qudt/applicableUnit",
      "@type" : "@id"
    },
    "label" : {
      "@id" : "http://www.w3.org/2000/01/rdf-schema#label"
    },
    "isoNormativeReference" : {
      "@id" : "http://qudt.org/schema/qudt/isoNormativeReference",
      "@type" : "http://www.w3.org/2001/XMLSchema#anyURI"
    },
    "comment" : {
      "@id" : "http://www.w3.org/2000/01/rdf-schema#comment"
    },
    "broader" : {
      "@id" : "http://www.w3.org/2004/02/skos/core#broader",
      "@type" : "@id"
    },
    "description" : {
      "@id" : "http://purl.org/dc/terms/description",
      "@type" : "http://qudt.org/schema/qudt/LatexString"
    },
    "latexDefinition" : {
      "@id" : "http://qudt.org/schema/qudt/latexDefinition",
      "@type" : "http://qudt.org/schema/qudt/LatexString"
    },
    "plainTextDescription" : {
      "@id" : "http://qudt.org/schema/qudt/plainTextDescription"
    },
    "symbol" : {
      "@id" : "http://qudt.org/schema/qudt/symbol"
    },
    "informativeReference" : {
      "@id" : "http://qudt.org/schema/qudt/informativeReference",
      "@type" : "http://www.w3.org/2001/XMLSchema#anyURI"
    },
    "hasDimensionVector" : {
      "@id" : "http://qudt.org/schema/qudt/hasDimensionVector",
      "@type" : "@id"
    },
    "isDefinedBy" : {
      "@id" : "http://www.w3.org/2000/01/rdf-schema#isDefinedBy",
      "@type" : "@id"
    },
    "rdf" : "http://www.w3.org/1999/02/22-rdf-syntax-ns#",
    "owl" : "http://www.w3.org/2002/07/owl#",
    "xsd" : "http://www.w3.org/2001/XMLSchema#",
    "rdfs" : "http://www.w3.org/2000/01/rdf-schema#"
  }
}
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