1998•Transactions of the American Nuclear SocietyRequires access

Subcritical measurements of uranium shells

Charles A. Goulding, William L. Myers, Charles L. Hollas

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Abstract

The authors have begun a program of measuring the degree of subcriticality of highly enriched uranium (HEU) systems. They have used the Feynman variance technique and point kinetics to extract a value for k{sub eff}. The measurements were done with the Rocky Flats shells. For the bare uranium systems, the HEU was driven with an internal source of {sup 252}Cf, AmF, and AmBe. The two ({alpha},n) sources were chosen so that one (AmF) would be close to the neutron energy spectrum for fission and the other would have a much higher average energy. To reach higher multiplications, they reflected the HEU with metallic shells. For the reflected systems, the HEU was driven either by an internal (AmF) source or an external deuterium-tritium (D-T) neutron generator.

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What this paper is about

The authors have begun a program of measuring the degree of subcriticality of highly enriched uranium (HEU) systems. They have used the Feynman variance technique and point kinetics to extract a value for k{sub eff}. The measurements were done with the Rocky Flats shells. For the bare uranium systems, the HEU was driven with an internal source of {sup 252}Cf, AmF, and AmBe. The two ({alpha},n) sources were chosen so that one (AmF) would be close to the neutron energy spectrum for fission and the other would have a much higher average energy. To reach higher multiplications, they reflected the HEU with metallic shells. For the reflected systems, the HEU was driven either by an internal (AmF) source or an external deuterium-tritium (D-T) neutron generator.

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Available abstract

The authors have begun a program of measuring the degree of subcriticality of highly enriched uranium (HEU) systems. They have used the Feynman variance technique and point kinetics to extract a value for k{sub eff}. The measurements were done with the Rocky Flats shells. For the bare uranium systems, the HEU was driven with an internal source of {sup 252}Cf, AmF, and AmBe. The two ({alpha},n) sources were chosen so that one (AmF) would be close to the neutron energy spectrum for fission and the other would have a much higher average energy. To reach higher multiplications, they reflected the HEU with metallic shells. For the reflected systems, the HEU was driven either by an internal (AmF) source or an external deuterium-tritium (D-T) neutron generator.

Key concepts: Isotopes of uranium, Enriched uranium, Uranium, Fission, Uranium-238, Neutron generator, Uranium-235, Nuclear physics

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