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NRC looks to leverage previous approvals for large LWRs
During this time of resurging interest in nuclear power, many conversations have centered on one fundamental problem: Electricity is needed now, but nuclear projects (in recent decades) have taken many years to get permitted and built.
In the past few years, a bevy of new strategies have been pursued to fix this problem. Workforce programs that seek to laterally transition skilled people from other industries, plans to reuse the transmission infrastructure at shuttered coal sites, efforts to restart plants like Palisades or Duane Arnold, new reactor designs that build on the legacy of research done in the early days of atomic power—all of these plans share a common throughline: leveraging work already done instead of starting over from square one to get new plants designed and built.
Valeria T. G. Riccardo, Philip L. Andrew, Alan Sandford Kaye, Peter Knoll
Fusion Science and Technology | Volume 43 | Number 4 | June 2003 | Pages 493-502
Technical Paper | doi.org/10.13182/FST03-A296
Articles are hosted by Taylor and Francis Online.
In view of the modification to the Joint European Torus (JET) plasma facing components foreseen for the 2004 shutdown, the disruption design criteria for in-vessel components have been updated building on the operational experience with divertor plasmas gained since the early 1990s. In fast disruptions the largest contribution to the electromechanical loads comes from currents induced by the poloidal field change. This is proportional to the plasma current decay rate, the maximum of which is observed to be linear with the predisruption plasma current, as if the current quench in the fastest events has a fixed duration, around 10 ms. Usually vertical displacement events (VDEs) take place on a longer timescale. In these cases halo currents determine the worst loading condition. Analysis of recent VDE data confirmed the previously observed magnitude of asymmetries: toroidal peaking factor times ratio of average poloidal halo to initial plasma current up to 0.42.Experimental evidence to justify the new criteria and procedures for applying them to JET are included. The revised design criteria are discussed and compared with those used for the components already present in the JET vessel.