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Fusion Energy
This division promotes the development and timely introduction of fusion energy as a sustainable energy source with favorable economic, environmental, and safety attributes. The division cooperates with other organizations on common issues of multidisciplinary fusion science and technology, conducts professional meetings, and disseminates technical information in support of these goals. Members focus on the assessment and resolution of critical developmental issues for practical fusion energy applications.
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Latest News
First astatine-labeled compound shipped in the U.S.
The Department of Energy’s National Isotope Development Center (NIDC) on March 31 announced the successful long-distance shipment in the United States of a biologically active compound labeled with the medical radioisotope astatine-211 (At-211). Because previous shipments have included only the “bare” isotope, the NIDC has described the development as “unleashing medical innovation.”
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).