quantitykind:TotalMassStoppingPower

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

Type
Description

If a substance is compared in gaseous and solid form, then the linear stopping powers of the two states are very different just because of the different density. One therefore often divides S(E) by the density of the material to obtain the "Mass Stopping Power". The mass stopping power then depends only very little on the density of the material.

Properties
qudt:plainTextDescription
If a substance is compared in gaseous and solid form, then the linear stopping powers of the two states are very different just because of the different density. One therefore often divides S(E) by the density of the material to obtain the "Mass Stopping Power". The mass stopping power then depends only very little on the density of the material.
qudt:iec61360Code
0112/2///62720#UAD204
qudt:latexDefinition
$S_m = \frac{S}{\rho}$, where $S$ is the total linear stopping power and $\rho$ is the mass density of the sample.
Annotations
dcterms:description
If a substance is compared in gaseous and solid form, then the linear stopping powers of the two states are very different just because of the different density. One therefore often divides S(E) by the density of the material to obtain the "Mass Stopping Power". The mass stopping power then depends only very little on the density of the material.
rdfs:label
Total Mass Stopping Power(en)
View as:  CSV

Work in progress

RDF/XML
<rdf:RDF
    xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#"
    xmlns:j.0="http://qudt.org/schema/qudt/"
    xmlns:j.1="http://purl.org/dc/terms/"
    xmlns:owl="http://www.w3.org/2002/07/owl#"
    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/TotalMassStoppingPower">
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/ERG-CentiM2-PER-GM"/>
    <j.0:hasDimensionVector rdf:resource="http://qudt.org/vocab/dimensionvector/A0E0L4I0M0H0T-2D0"/>
    <j.0:latexDefinition rdf:datatype="http://qudt.org/schema/qudt/LatexString">$S_m = \frac{S}{\rho}$, where $S$ is the total linear stopping power and $\rho$ is the mass density of the sample.</j.0:latexDefinition>
    <j.0:plainTextDescription>If a substance is compared in gaseous and solid form, then the linear stopping powers of the two states are very different just because of the different density. One therefore often divides S(E) by the density of the material to obtain the "Mass Stopping Power". The mass stopping power then depends only very little on the density of the material.</j.0:plainTextDescription>
    <j.0:symbol>S_m</j.0:symbol>
    <rdfs:isDefinedBy rdf:resource="http://qudt.org/2.1/vocab/quantitykind"/>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/J-M2-PER-KiloGM"/>
    <j.0:informativeReference rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://en.wikipedia.org/wiki/Stopping_power_(particle_radiation)</j.0:informativeReference>
    <rdfs:label xml:lang="en">Total Mass Stopping Power</rdfs:label>
    <j.0:iec61360Code>0112/2///62720#UAD204</j.0:iec61360Code>
    <rdf:type rdf:resource="http://qudt.org/schema/qudt/QuantityKind"/>
    <j.1:description rdf:datatype="http://qudt.org/schema/qudt/LatexString">If a substance is compared in gaseous and solid form, then the linear stopping powers of the two states are very different just because of the different density. One therefore often divides S(E) by the density of the material to obtain the "Mass Stopping Power". The mass stopping power then depends only very little on the density of the material.</j.1:description>
    <j.0:isoNormativeReference rdf:datatype="http://www.w3.org/2001/XMLSchema#anyURI">http://www.iso.org/iso/catalogue_detail?csnumber=31895</j.0:isoNormativeReference>
    <j.0:applicableUnit rdf:resource="http://qudt.org/vocab/unit/EV-M2-PER-KiloGM"/>
  </rdf:Description>
</rdf:RDF>
TURTLE
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@prefix rdfs: <http://www.w3.org/2000/01/rdf-schema#> .
@prefix xsd: <http://www.w3.org/2001/XMLSchema#> .

<http://qudt.org/vocab/quantitykind/TotalMassStoppingPower>
  rdf:type <http://qudt.org/schema/qudt/QuantityKind> ;
  <http://purl.org/dc/terms/description> "If a substance is compared in gaseous and solid form, then the linear stopping powers of the two states are very different just because of the different density. One therefore often divides S(E) by the density of the material to obtain the \"Mass Stopping Power\". The mass stopping power then depends only very little on the density of the material."^^<http://qudt.org/schema/qudt/LatexString> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/ERG-CentiM2-PER-GM> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/EV-M2-PER-KiloGM> ;
  <http://qudt.org/schema/qudt/applicableUnit> <http://qudt.org/vocab/unit/J-M2-PER-KiloGM> ;
  <http://qudt.org/schema/qudt/hasDimensionVector> <http://qudt.org/vocab/dimensionvector/A0E0L4I0M0H0T-2D0> ;
  <http://qudt.org/schema/qudt/iec61360Code> "0112/2///62720#UAD204" ;
  <http://qudt.org/schema/qudt/informativeReference> "http://en.wikipedia.org/wiki/Stopping_power_(particle_radiation)"^^xsd:anyURI ;
  <http://qudt.org/schema/qudt/isoNormativeReference> "http://www.iso.org/iso/catalogue_detail?csnumber=31895"^^xsd:anyURI ;
  <http://qudt.org/schema/qudt/latexDefinition> "$S_m = \\frac{S}{\\rho}$, where $S$ is the total linear stopping power and $\\rho$ is the mass density of the sample."^^<http://qudt.org/schema/qudt/LatexString> ;
  <http://qudt.org/schema/qudt/plainTextDescription> "If a substance is compared in gaseous and solid form, then the linear stopping powers of the two states are very different just because of the different density. One therefore often divides S(E) by the density of the material to obtain the \"Mass Stopping Power\". The mass stopping power then depends only very little on the density of the material." ;
  <http://qudt.org/schema/qudt/symbol> "S_m" ;
  rdfs:isDefinedBy <http://qudt.org/2.1/vocab/quantitykind> ;
  rdfs:label "Total Mass Stopping Power"@en ;
.
JSON
{"resource":"Total Mass Stopping Power" 
 ,"qname":"quantitykind:TotalMassStoppingPower" 
 ,"uri":"http:\/\/qudt.org\/vocab\/quantitykind\/TotalMassStoppingPower" 
 ,"properties":["applicable unit":"unit:ERG-CentiM2-PER-GM" 
    ,"applicable unit":"unit:EV-M2-PER-KiloGM" 
    ,"applicable unit":"unit:J-M2-PER-KiloGM" 
    ,"description":"If a substance is compared in gaseous and solid form, then the linear stopping powers of the two states are very different just because of the different density. One therefore often divides S(E) by the density of the material to obtain the \"Mass Stopping Power\". The mass stopping power then depends only very little on the density of the material." 
    ,"description (plain text)":"If a substance is compared in gaseous and solid form, then the linear stopping powers of the two states are very different just because of the different density. One therefore often divides S(E) by the density of the material to obtain the \"Mass Stopping Power\". The mass stopping power then depends only very little on the density of the material." 
    ,"has dimension vector":"dimension:A0E0L4I0M0H0T-2D0" 
    ,"iec-61360 code":"0112\/2\/\/\/62720#UAD204" 
    ,"informative reference":"http:\/\/en.wikipedia.org\/wiki\/Stopping_power_(particle_radiation)" 
    ,"isDefinedBy":"&lt;http:\/\/qudt.org\/2.1\/vocab\/quantitykind&gt;" 
    ,"label":"Total Mass Stopping Power" 
    ,"latex definition":"$S_m = \\frac{S}{\\rho}$, where $S$ is the total linear stopping power and $\\rho$ is the mass density of the sample." 
    ,"normative reference (ISO)":"http:\/\/www.iso.org\/iso\/catalogue_detail?csnumber=31895" 
    ,"symbol":"S_m" 
    ,"type":"qudt:QuantityKind" 
    ]}
JSON-LD
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  "description" : "If a substance is compared in gaseous and solid form, then the linear stopping powers of the two states are very different just because of the different density. One therefore often divides S(E) by the density of the material to obtain the \"Mass Stopping Power\". The mass stopping power then depends only very little on the density of the material.",
  "applicableUnit" : [ "http://qudt.org/vocab/unit/ERG-CentiM2-PER-GM", "http://qudt.org/vocab/unit/J-M2-PER-KiloGM", "http://qudt.org/vocab/unit/EV-M2-PER-KiloGM" ],
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  },
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