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Division Spotlight
Thermal Hydraulics
The division provides a forum for focused technical dialogue on thermal hydraulic technology in the nuclear industry. Specifically, this will include heat transfer and fluid mechanics involved in the utilization of nuclear energy. It is intended to attract the highest quality of theoretical and experimental work to ANS, including research on basic phenomena and application to nuclear system design.
Meeting Spotlight
ANS Student Conference 2025
April 3–5, 2025
Albuquerque, NM|The University of New Mexico
Standards Program
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
Candidates for leadership provide statements: ANS Board of Directors
With the annual ANS election right around the corner, American Nuclear Society members will be going to the polls to vote for a vice president/president-elect, treasurer, and members-at-large for the Board of Directors. In January, Nuclear News published statements from candidates for vice president/president-elect and treasurer. This month, we are featuring statements from each nominee for the Board of Directors.
Dennis G. Perry, Margaret L. Simmons, James S. Gilmore
Nuclear Technology | Volume 33 | Number 1 | April 1977 | Pages 103-109
Technical Paper | Accelerator | doi.org/10.13182/NT77-A31767
Articles are hosted by Taylor and Francis Online.
The neutron flux generated at the main proton beam stop of the Los Alamos Clinton P. Anderson Meson Physics Facility (LAMPF) has unique properties of interest to materials radiation studies. Two of these properties—the total neutron flux and the neutron energy spectrum—were studied. The total neutron flux at the LAMPF radiation effects facility has been calculated by Monte Carlo techniques and measured by foil activation methods. The measurement compares well with the calculation and gives a total flux at the measurement position of 2 × 1011 n. mm−2 . s−1 at 1 mA of proton beam current. Later calculations at other locations show a flux of 1 × 1012 n . mm−2 . s−1.