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The division provides a forum for focused technical dialogue on thermal hydraulic technology in the nuclear industry. Specifically, this will include heat transfer and fluid mechanics involved in the utilization of nuclear energy. It is intended to attract the highest quality of theoretical and experimental work to ANS, including research on basic phenomena and application to nuclear system design.
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November 17–21, 2024
Orlando, FL|Renaissance Orlando at SeaWorld
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FERC rejects interconnection deal for Talen-Amazon data centers
The Federal Energy Regulatory Commission has denied plans for Talen Energy to supply additional on-site power to an Amazon Web Services’ data center campus from the neighboring Susquehanna nuclear plant in Pennsylvania.
Robert L. Bieri
Fusion Science and Technology | Volume 19 | Number 3 | May 1991 | Pages 752-757
Inertial Fusion | doi.org/10.13182/FST91-A29435
Articles are hosted by Taylor and Francis Online.
The SAFIRE (Systems Analysis for ICF Reactor Economics) code was adapted to model a power plant using a HYLIFE-II reactor chamber. The code was then used to examine the dependence of the plant capital costs and the busbar cost of electricity (COE) on a variety of design parameters (type of driver, chamber repetition rate, and net electric power). The results show the most attractive operating space for each set of driver/target assumptions and quantify the benefits of improvements in key design parameters. The basecase plant was a 1,000-MWe plant containing a reactor vessel driven by an induction linac heavy-ion accelerater, run at 8 Hz with a driver energy of 6.73 MJ and a target yield of 350 MJ. The total direct cost for this plant was $2.6 billion. (All costs in this paper are given in equivalent 1988 dollars.) The COE was 8.5 ¢/(kW·h). The COE and total capital costs for a 1,000-MWe base plant are nearly independent of the chosen combination of repetition rate and driver energy for a driver operating between 4 and 10 Hz. For comparison, the COE for a coal or future fission plant would be 4.5–5.5 ¢/(kW·h). The COE for a 1,000-MWe plant could be reduced to 7.5 ¢/(kW·h) by using advanced targets and could be cut to 6.5 ¢/(kW·h) with conventional targets, if the driver cost could be cut in half. There is a large economy of scale with heavy-ion-driven inertial confinement fusion (ICF) plants. A 2,000-MWe plant with a heavy-ion driver and a HYLIFE-II chamber would have a COE of only 5.8 ¢/(kW·h).