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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.
Takanori Kameyama, Tetsuo Matsumura, Motoyasu Kinoshita
Nuclear Technology | Volume 106 | Number 3 | June 1994 | Pages 334-341
Technical Paper | Nuclear Fuel Cycle | doi.org/10.13182/NT94-A34963
Articles are hosted by Taylor and Francis Online.
The peripheral region of a high burnup light water reactor (LWR) fuel pellet shows a microstructure that is different from the as-fabricated microstructure. The region where the microstructure change occurs (the rim region) is highly porous, and the original grains in the rim region are divided into much smaller subgrains. The electron probe microanalysis data of high burnup fuels indicate fission gas depletion in the rim region as well as in the central region. The burnup in the rim region is enhanced by built-up plutonium derived from a 238U self-shielding effect, which is called a rim effect. The rim effect accelerates microstructure change in the peripheral region. We developed a detailed burnup analysis code ANRB computing the rim effect in LWR fuels. We have verified the ANRB code performance with the data of the High Burnup Effects Program. The analysis shows that the microstructure change occurs where local burnup gets to the threshold burnup of 70 to 80 MWd/kg U in both pressurized water reactor and boiling water reactor types of fuels. The threshold burnup never changes with the plutonium/uranium burnup ratio or fission rate during the irradiation. The storage of radiation damage is expected to cause the microstructure change.