Published July 1993 | Version v1
Report Restricted

Summary of ionizing and displacive irradiation fields in various facilities

  • 1. Oak Ridge National Laboratory, TN (United States)
  • 2. Pacific Northwest Laboratory, Richland, WA (United States)

Description

Calculations have been performed to estimate the ionizing and displacive irradiation fields that will occur in ceramics during irradiation in accelerators and fission and fusion reactors. A useful measure of the relative strength of ionizing vs. displasive radiation is the ratio of the absorbed ionizing dose to the displacement damage dose, which in the case of ion irradiation is equal to the ratio of the electronic stopping power to the nuclear stopping power. In ceramics such as Al2O3, this ratio is about 20 at a fusion reactor first wall, and has a typical value of about 100 in a fusion reactor blanket region and in mixed spectrum reactors such as HFIR. Particle accelerator sources typically have much higher ionizing to displacive radiation ratios, ranging from about 2000 for 1 MeV protons to >10,000 for 1 MeV electrons

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Part of:
Fusion reactor materials semiannual progress report for the period ending March 31, 1993

Additional details

Publishing Information

Imprint Title
Fusion reactor materials semiannual progress report for the period ending March 31, 1993
Imprint Pagination
524 p.
Journal Page Range
p. 74-78.
Report number
DOE/ER--0313/14

INIS

Country of Publication
United States
Country of Input or Organization
United States
INIS RN
25054097
Subject category
S70: PLASMA PHYSICS AND FUSION TECHNOLOGY; S36: MATERIALS SCIENCE;
Resource subtype / Literary indicator
Progress Report
Descriptors DEI
ALUMINIUM OXIDES; COULOMB IONIZATION; ELECTRONS; IONS; IRRADIATION; NEUTRONS; PROGRESS REPORT; STOPPING POWER
Descriptors DEC
ALUMINIUM COMPOUNDS; BARYONS; CHALCOGENIDES; CHARGED PARTICLES; DOCUMENT TYPES; ELEMENTARY PARTICLES; FERMIONS; HADRONS; IONIZATION; LEPTONS; NUCLEONS; OXIDES; OXYGEN COMPOUNDS

Optional Information