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Nuclear Nonproliferation Policy
The mission of the Nuclear Nonproliferation Policy Division (NNPD) is to promote the peaceful use of nuclear technology while simultaneously preventing the diversion and misuse of nuclear material and technology through appropriate safeguards and security, and promotion of nuclear nonproliferation policies. To achieve this mission, the objectives of the NNPD are to: Promote policy that discourages the proliferation of nuclear technology and material to inappropriate entities. Provide information to ANS members, the technical community at large, opinion leaders, and decision makers to improve their understanding of nuclear nonproliferation issues. Become a recognized technical resource on nuclear nonproliferation, safeguards, and security issues. Serve as the integration and coordination body for nuclear nonproliferation activities for the ANS. Work cooperatively with other ANS divisions to achieve these objective nonproliferation policies.
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Conference on Nuclear Training and Education: A Biennial International Forum (CONTE 2025)
February 3–6, 2025
Amelia Island, FL|Omni Amelia Island Resort
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
Senate committee hears from energy secretary nominee Chris Wright
Wright
Chris Wright, president-elect Trump’s pick to lead the U.S. Department of Energy, spent hours today fielding questions from members of the U.S. Senate’s committee on Energy and Natural Resources.
During the hearing, Wright—who’s spent most of his career in fossil fuels—made comments in support of nuclear energy and efforts to expand domestic generation in the near future. Asked what actions he would take as energy secretary to improve the development and deployment of SMRs, Wright said: “It’s a big challenge, and I’m new to government, so I can’t list off the five levers I can pull. But (I’ve been in discussions) about how to make it easier to research, to invest, to build things. The DOE has land at some of its facilities that can be helpful in this regard.”
Pedro A. Landeyro, Tadeusz Zoltowski
Nuclear Science and Engineering | Volume 104 | Number 2 | February 1990 | Pages 183-187
Technical Note | doi.org/10.13182/NSE90-A23714
Articles are hosted by Taylor and Francis Online.
The aim of the research was to study the monitoring of keff in some steps of fissile material processing. Two sets of experimental tests were performed. In the first one, variable gradients of concentration were modeled, while in the second one (uniform) the tank was filled at different levels with ura-nyl-nitrate solution having 45 g U/ (80 wt% enriched in 235U). Another uniform configuration series was calculated to cover a range of keff not far from criti-cality. In the last computations, all the calculational models were used to represent experiments in which only the source position changes from the axis of the setup to the position 0.5 cm out of the external surface of the tank. The keff calculations were performed with the KENO-IV Monte Carlo code. The flux computations were carried out with the MORSE C. G. code. The dependence between k∞ and Mepi (the external source epithermal multiplication) previously established was used for the analysis of experimental and calculational tests. Excellent agreement between neutron multiplication or epithermal neutron multiplication measured and calculated values was found. The agreement between keff values obtained from the measured and calculated epithermal neutron multiplication data and KENO-IV results improves with the increase of keff values. The relative differences are within the Monte Carlo calculation error range (∼10%) for keff values >0.65 for the axially located source configurations, >0.37 for configurations when neutron source was located externally and fissile material distributed uniformly, and >0.66 when neutron source was located externally and for configurations with fissile material concentration gradients.