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Simulation of shell pellet injection strategies for ITER-scale tokamaks
Abstract
Dispersive shell pellet (DSP) injection is considered as an alternative to shattered pellet injection as a disruption mitigation system for ITER, and strategies for penetration of a shell pellet into ITER are modeled with the 3D MHD code NIMROD. Because the high plasma temperatures lead to rapid ablation of the shell, delivery of the dispersive payload to the core of ITER will be very challenging. Two strategies to increase payload delivery depth are modeled: first, multiple staggered pellets are simulated in DIII-D, to assess the ability for one DSP to "piggy-back" on another to reach deeper into the core; second, DSP injection after pre-dilution-cooling with deuterium is simulated in ITER, in order to reduce the plasma temperature before shell pellet arrival. The DIII-D simulations show that a second, slower pellet can penetrate much deeper once the release of the first payload strongly cools the mid-radius region. When the pellets are staggered, deeper penetration of the second pellet leads to higher radiation fraction and larger runaway electron loss fraction, consistent with single pellet results. However, simultaneously released pellets at mid-radius that do not trigger a large n=1 mode produce an even higher radiation fraction. The ITER simulations show that an inside-outmore »
- Authors:
-
- Fiat Lux, San Diego, CA (United States)
- Publication Date:
- Research Org.:
- General Atomics, San Diego, CA (United States)
- Sponsoring Org.:
- USDOE Office of Science (SC), Fusion Energy Sciences (FES); USDOE Office of Science (SC), Basic Energy Sciences (BES). Scientific User Facilities (SUF)
- OSTI Identifier:
- 1989661
- Grant/Contract Number:
- FC02-04ER54698; FG02-95ER54309; AC02-05CH11231
- Resource Type:
- Accepted Manuscript
- Journal Name:
- Plasma Physics and Controlled Fusion
- Additional Journal Information:
- Journal Volume: 65; Journal Issue: 9; Journal ID: ISSN 0741-3335
- Publisher:
- IOP Science
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 70 PLASMA PHYSICS AND FUSION TECHNOLOGY; simulations; ITER; disruption mitigation; MHD; tokamak; shell pellet
Citation Formats
Izzo, Valerie A. Simulation of shell pellet injection strategies for ITER-scale tokamaks. United States: N. p., 2023.
Web. doi:10.1088/1361-6587/ace6d4.
Izzo, Valerie A. Simulation of shell pellet injection strategies for ITER-scale tokamaks. United States. https://doi.org/10.1088/1361-6587/ace6d4
Izzo, Valerie A. Wed .
"Simulation of shell pellet injection strategies for ITER-scale tokamaks". United States. https://doi.org/10.1088/1361-6587/ace6d4.
@article{osti_1989661,
title = {Simulation of shell pellet injection strategies for ITER-scale tokamaks},
author = {Izzo, Valerie A.},
abstractNote = {Dispersive shell pellet (DSP) injection is considered as an alternative to shattered pellet injection as a disruption mitigation system for ITER, and strategies for penetration of a shell pellet into ITER are modeled with the 3D MHD code NIMROD. Because the high plasma temperatures lead to rapid ablation of the shell, delivery of the dispersive payload to the core of ITER will be very challenging. Two strategies to increase payload delivery depth are modeled: first, multiple staggered pellets are simulated in DIII-D, to assess the ability for one DSP to "piggy-back" on another to reach deeper into the core; second, DSP injection after pre-dilution-cooling with deuterium is simulated in ITER, in order to reduce the plasma temperature before shell pellet arrival. The DIII-D simulations show that a second, slower pellet can penetrate much deeper once the release of the first payload strongly cools the mid-radius region. When the pellets are staggered, deeper penetration of the second pellet leads to higher radiation fraction and larger runaway electron loss fraction, consistent with single pellet results. However, simultaneously released pellets at mid-radius that do not trigger a large n=1 mode produce an even higher radiation fraction. The ITER simulations show that an inside-out TQ can be produced with a payload release just inside of the q=2 surface, which is achieved at a speed of 800 m/s after pre-dilution cooling. Although stochastization of the core leads to a complete thermal quench, the edge flux surfaces are surprisingly robust in the ITER simulations, regardless of payload release location. As a result, runaway electron losses would not be expected.},
doi = {10.1088/1361-6587/ace6d4},
journal = {Plasma Physics and Controlled Fusion},
number = 9,
volume = 65,
place = {United States},
year = {Wed Jul 26 00:00:00 EDT 2023},
month = {Wed Jul 26 00:00:00 EDT 2023}
}
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