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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.
Mansoor Siddique, Michael W. Golay, Mujid S. Kazimi
Nuclear Technology | Volume 102 | Number 3 | June 1993 | Pages 386-402
Technical Paper | Heat Transfer and Fluid Flow | doi.org/10.13182/NT93-A17037
Articles are hosted by Taylor and Francis Online.
An experimental investigation has been conducted to determine the local condensation heat transfer coefficient (HTC) of steam in the presence of air or helium flowing downward inside a 46-mm-i.d. vertical tube. The gas-steam mixture flow rate was measured with a calibrated vortex flowmeter before it entered the 2.54-m-long test condenser. Cooling water flow rate in an annulus around the tube was measured with a calibrated rotameter. Temperatures of the cooling water, the gas-steam mixture, and the tube inside and outside surfaces were measured at 0.3-m intervals in the test condenser. Inlet and exit pressures and temperatures of the gas-steam mixture and of the cooling water were also measured. The local heat flux was obtained from the slope of the coolant axial temperature profile and the coolant mass flow rate. For the air-stream experiments, the ranges of the test variables were as follows: mixture inlet temperatures of 100,120, and 140°C; inlet air mass fraction of 10 to 35%; and mixture inlet Reynolds number of ∼5000 to 22 700. For the helium-steam experiments, the ranges of the test variables were as follows: mixture inlet temperatures of 100, 120, and 140°C; inlet helium mass fraction of 2 to 10%; and mixture inlet Reynolds number of ∼5000 to 11400. The local HTC varied from 100 to ∼25 000 W/m2·°C. The local Nusselt number calculated from the obtained data was correlated in terms of the local mixture Reynolds number, Jakob number, Schmidt number, and gas mass fractions. It was found that for the same mass fraction of the noncondensable gas, compared with air, helium has a more inhibiting effect on the heat transfer, but for the same molar ratio, air was found to be more inhibiting.