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Absorbed dose
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===Dose computation=== The absorbed dose is equal to the radiation exposure (ions or [[coulomb|C]]/kg) of the radiation beam multiplied by the ionization energy of the medium to be ionized. For example, the ionization energy of dry air at 20 Β°C and 101.325 [[pascal (unit)|kPa]] of pressure is {{val|33.97|0.05|u=J/C}}.<ref>{{Cite journal|last1=Boutillon|first1=M|last2=Perroche-Roux|first2=A M|date=1987-02-01|title=Re-evaluation of the W value for electrons in dry air|url=http://stacks.iop.org/0031-9155/32/i=2/a=005?key=crossref.39f54fc0a89c599c170f539f60fb5d2f|journal=Physics in Medicine and Biology|volume=32|issue=2|pages=213β219|doi=10.1088/0031-9155/32/2/005|bibcode=1987PMB....32..213B|s2cid=250751778|issn=0031-9155|url-access=subscription}}</ref> (33.97 eV per ion pair) Therefore, an exposure of {{val|2.58|e=-4|u=C/kg}} (1 [[roentgen (unit)|roentgen]]) would deposit an absorbed dose of {{val|8.76|e=-3|u=J/kg}} (0.00876 Gy or 0.876 rad) in dry air at those conditions. When the absorbed dose is not uniform, or when it is only applied to a portion of a body or object, an absorbed dose representative of the entire item can be calculated by taking a mass-weighted average of the absorbed doses at each point. More precisely,{{sfn | ICRP | 2007 | p=1 }} <math display=block>\overline{D_T} = \frac{\displaystyle \int_{T} D(x,y,z) \, \rho(x,y,z) \, dV} {\displaystyle \int_{T} \rho(x,y,z) \, dV}</math> Where *<math>\overline{D_T}</math> is the mass-averaged absorbed dose of the entire item <math>T</math>; *<math>T</math> is the item of interest; *<math>D(x,y,z)</math> is the absorbed dose density (absorbed dose per unit volume) as a function of location; *<math>\rho(x,y,z)</math> is the density (mass per unit volume) as a function of location; *<math>V</math> is volume.
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