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The human factor in licensing and operating the next generation of nuclear plants
As human factors specialists working at the intersection of human performance and nuclear operations, we are witnessing one of the nuclear sector’s most significant transitions in decades. The emergence of small modular reactors, microreactors, and other advanced designs is reshaping the industry’s landscape. Digital instrumentation and controls, passive safety systems, and increased automation are creating opportunities for greater safety margins and more flexible operation. These same features also fundamentally redefine what it means to “operate” a nuclear plant. Interactions among human roles, automation, and passive systems shape how people maintain awareness, exercise judgment, and intervene when necessary. These developments affect both operational realities and the regulatory foundations on which nuclear safety is built.
W. B. Doub
Nuclear Science and Engineering | Volume 10 | Number 4 | August 1961 | Pages 299-307
doi.org/10.13182/NSE61-A15371
Articles are hosted by Taylor and Francis Online.
An approximate heuristic expression for the particle self-shielding factor for a set of purely absorbing spheres of radius r and volume fraction V well mixed with another set of non-absorbing spheres has been derived. The resulting expression has been experimentally verified using transmission data at several incident neutron energies for a plate-type sample containing a mixture of aluminum and boron-carbide spheres with nominal diameters 85 ± 15µ. The boron-carbide spheres occupied about 37% of the sample volume. The transmission was measured at energies ranging from 0.03 to 1.2 ev using a crystal neutron spectrometer. Since, however, the sample contained boron-carbide spheres with a distribution of diameters, the experimental self-shielding factors are “average” values. It is shown, using an approximate model, that a plausible theoretical self-shielding factor is a volume weighted average of the self-shielding factors for the spheres of diameters, d1, d2, d3, … . The particle self-shielding factors derived by several other authors have also been compared with the present experimental results. The Hurwitz-Zweifel expression (1) gives quite bad agreement, though this is expected because of the high volume fraction of poison in the sample. The Burrus expression (2, 3) gives much better agreement though not as good as the expression derived in this paper.