@prefix isq: <https://w3id.org/standards/isq/ontologies/core/> .
@prefix smart: <https://example.org/smart-sdu/> .
@prefix rdf: <http://www.w3.org/1999/02/22-rdf-syntax-ns#> .
@prefix dcterms: <http://purl.org/dc/terms/> .
@prefix skos: <http://www.w3.org/2004/02/skos/core#> .

<isq:t10-87>
  a isq:Entry ;
  rdf:type isq:Quantity ;
  rdf:type smart:TermEntry ;
  dcterms:identifier "10-87" ;
  skosxl:prefLabel "mass energy-transfer coefficient"@en ;
  skosxl:altLabel "mu_\"tr\"//rho"@en ;
  skos:definition "for ionizing uncharged particles of a given type and energy, the differential quotient of stem:[R_\"tr\"] with respect to stem:[l]:\n\n[stem%unnumbered]\n++++\n(mu_\"tr\")/rho = 1/rho 1/R (\"d\"R_\"tr\")/(\"d\"l)\n++++\n\nwhere stem:[R_\"tr\"] is the mean energy (<<iso80000-5>>) that is transferred to kinetic energy (<<iso80000-4>>) of charged particles by interactions of the uncharged particles of incident radiant energy stem:[R] (<<t10-45>>) in traversing a distance (<<iso80000-3>>) stem:[l] in the material of density (<<iso80000-4>>) stem:[rho], divided by stem:[rho] and stem:[R]\n"@en ;
  smart:hasBindingnessType "bindingness-type:normative" ;
  dcterms:isPartOf <isq:part-10> ;
  isq:hasUnit [
    skos:notation "kg^(-1)*m^2" ;
    skosxl:prefLabel "square metre per kilogram"@en
  ] ;
  skos:note "stem:[mu_\"tr\"//rho = dot K//ii(Psi)], where stem:[dot K] is kerma rate (<<t10-86.2>>) and stem:[ii(Psi)] is energy fluence rate (<<t10-47>>).\n\nThe quantity:\n\n[stem%unnumbered]\n++++\nmu_\"en\"//rho = (mu_\"tr\"//rho)(1-g)\n++++\n\nwhere stem:[g] is mean fraction of the kinetic energy of the liberated charged particles that is lost in radiative processes in the material, is called mass energy-absorption coefficient.\n\nThe mass energy-absorption coefficient of a compound material depends on the stopping power of the material. Thus, its evaluation cannot, in principle, be reduced to a simple summation of the mass energy-absorption coefficient of the atomic constituents. Such a summation can provide an adequate approximation when the value of stem:[g] is sufficiently small.\n\nIn report 85a of the ICRU a definition with an equivalent meaning is given as:\n\nThe mass energy-transfer coefficient, stem:[mu_\"tr\"//rho], of a material, for uncharged particles of a given type and energy, is the quotient of stem:[\"d\"R_\"tr\"//R] by stem:[rho \"d\"l], where stem:[\"d\"R_\"tr\"] is the mean energy that is transferred to kinetic energy of charged particles by interactions of the uncharged particles of incident radiant energy stem:[R] in traversing a distance stem:[\"d\"l] in the material of density stem:[rho]:\n\n[stem%unnumbered]\n++++\n(mu_\"tr\")/rho = 1/(rho \"d\"l) (\"d\"R_\"tr\")/R.\n++++\n"@en ;
  iso:urn <urn:iso:std:iso:80000:-10:ed-2:en:item:10-87> .
