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Nuclear Installations Safety
Devoted specifically to the safety of nuclear installations and the health and safety of the public, this division seeks a better understanding of the role of safety in the design, construction and operation of nuclear installation facilities. The division also promotes engineering and scientific technology advancement associated with the safety of such facilities.
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International Conference on Mathematics and Computational Methods Applied to Nuclear Science and Engineering (M&C 2025)
April 27–30, 2025
Denver, CO|The Westin Denver Downtown
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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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Ariz. governor vetoes “fast track” bill for nuclear
Gov. Katie Hobbs put the brakes on legislation that would have eliminated some of Arizona’s regulations and oversight of small modular reactors, technology that is largely under consideration by data centers and heavy industrial power users.
David B. Reister
Nuclear Science and Engineering | Volume 46 | Number 2 | November 1971 | Pages 197-202
Technical Paper | doi.org/10.13182/NSE71-A22353
Articles are hosted by Taylor and Francis Online.
Optimum upper and lower flux bounds are sought for a general space-time reactor problem. The bounds are much narrower than previous bounds. Each bound is a sum of the products of known spatial modes and unknown time-dependent amplitude functions. To determine a bound, the amplitude functions must satisfy certain inequalities given by a comparison theorem of the Nagumo-Westphal type. An optimum bound is one that satisfies the inequalities and minimizes a “payoff function. In this paper, the payoff function is the weighted average of the magnitude of the bound at several points in the reactor. It is shown that an optimum bound can be determined by solving a linear programming problem at each time step. (Linear programming can be used even if there is feedback and the problem is nonlinear.) Using linear programming theory it is shown that an optimum bound always exists, although it may not be unique. Furthermore, an optimum bound satisfies the original space-time equation at each point in the reactor sampled by the payoff function. In an example, narrow bounds are determined for a difficult example in which the spatial shape of the flux changes radically with time.