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Accelerator Applications
The division was organized to promote the advancement of knowledge of the use of particle accelerator technologies for nuclear and other applications. It focuses on production of neutrons and other particles, utilization of these particles for scientific or industrial purposes, such as the production or destruction of radionuclides significant to energy, medicine, defense or other endeavors, as well as imaging and diagnostics.
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2024 ANS Annual Conference
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Las Vegas, NV|Mandalay Bay Resort and Casino
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The Standards Committee is responsible for the development and maintenance of voluntary consensus standards that address the design, analysis, and operation of components, systems, and facilities related to the application of nuclear science and technology. Find out What’s New, check out the Standards Store, or Get Involved today!
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Latest News
Can hydrogen be the transportation fuel in an otherwise nuclear economy?
Let’s face it: The global economy should be powered primarily by nuclear power. And it probably will by the end of this century, with a still-significant assist from renewables and hydro. Once nuclear systems are dominant, the costs come down to where gas is now; and when carbon emissions are reduced to a small portion of their present state, it will become obvious that most other sources are only good in niche settings. I mean, why use small modular reactors to load-follow when they can just produce that power instead of buffering it?
Barbora Gulejová, Richard Pitts, David Tskhakaya, David Coster
Fusion Science and Technology | Volume 60 | Number 1 | July 2011 | Pages 48-55
doi.org/10.13182/FST11-A12404
Articles are hosted by Taylor and Francis Online.
Although the most complex currently available fluid-neutral Monte-Carlo plasma boundary code package, SOLPS, has been a major player in the ITER divertor design, it has not yet been systematically used for the study of kinetic phenomena such as ELM transients. This paper investigates the relevance of fluid code results for transients, in particular at the targets where kinetic effects are most manifest, by comparing power and particle fluxes at the targets from SOLPS5 time-dependent simulations of TCV Type III ELMs with those obtained from dedicated Particle-in-Cell (PiC) kinetic transport code (BIT1) simulations. Although reasonable agreement is found in terms of the absolute magnitude of total heat fluxes, the arrival of the ion pulse at the target from upstream is significantly faster in SOLPS than expected on the basis of sonic transit times (as also seen in PiC). Adjustments of kinetic heat flux limiters to render the heat fluxes more convective in SOLPS are necessary in order to correct for this discrepancy. Moreover, because SOLPS does not account for the transfer of heat from electrons to ions inside the sheath, correction terms to the electron and ion power fluxes at the targets are required in SOLPS in order to better match PiC results. However, it does not appear possible within the scope of these sensitivity studies to simultaneously achieve expected delays and ion-electron power sharing in the fluid simulations.