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As executive vice president for industry strategy at the Institute of Nuclear Power Operations, Jeff Place leads INPO’s industry-facing work, engaging directly with chief nuclear officers.
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.