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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.
Shurong Ding, Yongzhong Huo
Nuclear Technology | Volume 163 | Number 3 | September 2008 | Pages 416-425
Technical Paper | Fuel Cycle and Management | doi.org/10.13182/NT08-A3999
Articles are hosted by Taylor and Francis Online.
A metal-matrix dispersion fuel plate is considered. Taking account of the actual geometry, a special three-dimensional representative volume element is developed according to the particle distributions, which might characterize not only the macro deformation along the thickness but also the micro stress-strain fields. An elastoplastic analysis using the finite element method is carried out for the thermal-mechanical behaviors induced only by the thermal effects. The distributions of the thermal stresses at the fuel particles and the matrix are given, and the effects of the surface heat transfer coefficients, the heat generation rates of the fuel particles, and the degraded conductivities of the fuel particles along with the burnup on the stresses and the size variations of the plate thickness are investigated. The research results indicate that the internal stress distributions are not spherically symmetrical. With increasing surface heat transfer coefficients, the first principal stresses at the particles and the matrix both fall, and the thickness increments decrease. The first principal stresses at the fuel particles and the matrix both grow with increasing heat generation rates, and the thickness variations linearly increase. With decrease of the thermal conductivities of the fuel particles, the first principal stresses at the matrix increase, and the relative stresses at the particles decrease.