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CLEAN SMART bill reintroduced in Senate
Senators Ben Ray Luján (D., N.M.) and Tim Scott (R., S.C.) have reintroduced legislation aimed at leveraging the best available science and technology at U.S. national laboratories to support the cleanup of legacy nuclear waste.
The Combining Laboratory Expertise to Accelerate Novel Solutions for Minimizing Accumulated Radioactive Toxins (CLEAN SMART) Act, introduced on February 11, would authorize up to $58 million annually to develop, demonstrate, and deploy innovative technologies, targeting reduced costs and safer, faster remediation of sites from the Manhattan Project and Cold War.
L. D. Philipp, N. C. Hoitink, W. G. Spear, M. R. Wood
Nuclear Technology | Volume 20 | Number 1 | October 1973 | Pages 51-59
Technical Paper | Instrument | doi.org/10.13182/NT73-A31333
Articles are hosted by Taylor and Francis Online.
Electron drift velocity, a function of gas composition, electric field, and pressure, represents the most important design parameter for optimization of fission-counter collection time. References in the literature provide a significant source of information on drift velocities for various gases, but the information does not extend to sufficiently high electric field/pressure (E/p) ratios for use with the high-sensitivity fission counters under consideration. The data obtained for this investigation and reported here extend the drift-velocity data for argon-nitrogen mixtures to E/p regions useful for present design considerations, and at the same time compare detector performance in a high gamma field (106 R/h) with the various gas mixtures employed. Six combinations of argon-nitrogen ranging from 1 to 15% nitrogen were included in the tests. Although several other gas mixtures, such as argon-methane and argon-CO2, provide faster drift velocities, only argon-nitrogen has proven stable at the high neutron exposure levels anticipated for the Fast Flux Test Facility (1018 n/cm2). Performance comparisons show that for 800-Vdc operation the neutron counting sensitivity for Ar - 10% N2 exceeds that for Ar - 1% N2 (the fill gas most commonly used) by over a factor of 2. Corresponding collection times decreased from 160 nsec for the Ar - 1% N2 mixture to 80 nsec for the Ar - 10% N2 combination. For specific applications, it may be required to limit the voltage to <800 Vdc. The curves provide information to permit selection of the best gas mixture for a given bias voltage requirement.