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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.
Bassam I. Shamoun, Michael L. Corradini
Nuclear Technology | Volume 115 | Number 1 | July 1996 | Pages 35-45
Technical Paper | Nuclear Reactor Safety | doi.org/10.13182/NT96-A35273
Articles are hosted by Taylor and Francis Online.
Experimental observation has shown that the assumption of complete fuel fragmentation in a vapor explosion by the shock adiabatic thermodynamic model results in predicting upper bounds for the shock pressure, propagation velocity, and work output. This model has been modified by considering the condition where the assumption of complete fragmentation of the fuel is relaxed. A methodology is adopted using experimental values of the shock pressure and propagation velocity to estimate the initial mixture conditions of the experiment and the mass fraction of the materials participating in the explosion. Analysis of a steady-state subcritical vapor explosion in one dimension has been carried out by applying the conservation laws of mass, momentum, and energy and the appropriate equation of state for a homogeneous mixture of molten tin and water. The KROTOS-21 experiment, conducted at the Joint Research Center at Ispra, Italy, was used as the initial benchmark experiment in this analysis. A quasisteady explosion pressure of ∼3 MPa and a propagation velocity of ∼200 m/s were obtained in this experiment. Using this model, the estimated minimum mass of the fragmented fuel was found to be 0.21 kg (3.2%) of the total mass of the fuel. The predicted work output by this model corresponding to the aforementioned fragmented fuel mass was found to be 9.8 kJ. The estimated initial void fraction of the vapor was found to be 11.5%. In these analyses, a comparison is made of the various possible closure relations applied to the detonation wave theory for a vapor explosion and associated concerns of model stability in the two-phase region.