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Accelerator Applications
The division was organized to promote the advancement of knowledge of the use of particle accelerator technologies for nuclear and other applications. It focuses on production of neutrons and other particles, utilization of these particles for scientific or industrial purposes, such as the production or destruction of radionuclides significant to energy, medicine, defense or other endeavors, as well as imaging and diagnostics.
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2024 ANS Winter Conference and Expo
November 17–21, 2024
Orlando, FL|Renaissance Orlando at SeaWorld
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The Standards Committee is responsible for the development and maintenance of voluntary consensus standards that address the design, analysis, and operation of components, systems, and facilities related to the application of nuclear science and technology. Find out What’s New, check out the Standards Store, or Get Involved today!
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Latest News
FERC rejects interconnection deal for Talen-Amazon data centers
The Federal Energy Regulatory Commission has denied plans for Talen Energy to supply additional on-site power to an Amazon Web Services’ data center campus from the neighboring Susquehanna nuclear plant in Pennsylvania.
R. K. Choudhury, R. G. Thomas, A. K. Mohanty, S. S. Kapoor
Nuclear Science and Engineering | Volume 169 | Number 3 | November 2011 | Pages 334-339
Technical Note | doi.org/10.13182/NSE10-62
Articles are hosted by Taylor and Francis Online.
Calculations of the yield of neutrons due to the interaction of protons on a deuterium gas target have been carried out for the primary p - d breakup reaction as well as for the secondary processes due to nuclear reactions induced by the elastically scattered protons and deuterons. The experimental conditions of Bowman et al. reported in a recent work were simulated with respect to the measurements of neutron yields in the proton energy range 7 to 17 MeV. It is found that the primary breakup reaction is the main source of neutron production and the contribution to the neutron yield from the secondary processes is quite small, being of the order of 1% to 2%. Thus, the discrepancy reported by Bowman et al. between the measured neutron yields and the theoretical calculations based on the primary breakup reaction alone cannot be explained by the inclusion of secondary processes. The possible reasons for the observed discrepancy are discussed. The calculations were extended up to Ep = 100 MeV. The conclusion drawn by Bowman et al. regarding the energy cost per neutron at Ep = 100 MeV by extrapolating the empirical function fitted to the experimental data measured up to 17 MeV is not borne out by the present calculations.