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Xenon construction materials

The choice of source material is a difficult problem. Hard radiation is required (to achieve high penetration through the electrolyte solution) but hard X-ray photons are difficult to detect in a proportional counter, requiring the use of high pressure and expensive xenon gas. This is acceptable with a sealed detector but it means that the construction materials must be carefully chosen to be clean, or the detector gas will soon become contaminated. Softer radiation is much easier to detect, and, for example, for Cu Ka photons reasonable detection efficiencies are obtained with Ar at atmospheric pressure. All the results reported here were obtained with a Cu Ka source, which limits the solution pathlength to a few tenths of a millimeter. This clearly makes cell design critical. For Mo Ka radiation, considerably thicker solution layers would be acceptable. [Pg.22]

Gaseous neon, krypton, and xenon are noncorrosive and inert, so they may be contained in systems constructed of any common metals designed to withstand safely the pressures involved. At the temperatures encountered with liquid neon, krypton, and xenon, ordinary carbon steels and most alloy steels lose their ductility and are considered unsafe for use with these cryogenic liquids. Satisfactory materials for use with liquid neon, krypton, and xenon include austenitic stainless steel (for example types 304 and 316) and other nickel-chromium alloys, copper. Monel, brass, and aluminum. [Pg.589]


See other pages where Xenon construction materials is mentioned: [Pg.540]    [Pg.2249]    [Pg.330]    [Pg.663]   
See also in sourсe #XX -- [ Pg.552 ]




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