Dispersive shell pellet injection modeling and validation for DIII-D disruption mitigation

2021 ◽  
Vol 28 (8) ◽  
pp. 082502
Author(s):  
V. A. Izzo
2021 ◽  
Author(s):  
You Li ◽  
Zhong yong Chen ◽  
Wei Yan ◽  
Yu Wei ◽  
Ruihai Tong ◽  
...  

2021 ◽  
Author(s):  
Larry R Baylor ◽  
Steve J Meitner ◽  
Trey E Gebhart ◽  
John B. O. Caughman ◽  
Daisuke Shiraki ◽  
...  

2019 ◽  
Vol 59 (6) ◽  
pp. 066008 ◽  
Author(s):  
L.R. Baylor ◽  
S.J. Meitner ◽  
T.E. Gebhart ◽  
J.B.O. Caughman ◽  
J.L. Herfindal ◽  
...  

2021 ◽  
Author(s):  
Stefan Jachmich ◽  
Uron Kruezi ◽  
Michael Lehnen ◽  
Matteo Baruzzo ◽  
Larry R Baylor ◽  
...  

Abstract A series of experiments have been executed at JET to assess the efficacy of the newly installed Shattered Pellet Injection (SPI) system in mitigating the effects of disruptions. Issues, important for the ITER disruption mitigation system, such as thermal load mitigation, avoidance of runaway electron formation, radiation asymmetries during thermal quench mitigation, electromagnetic load control and runaway electron energy dissipation have been addressed over a large parameter range. The efficiency of the mitigation has been examined for the various SPI injection strategies. The paper summarises the results from these JET SPI experiments and discusses their implications for the ITER disruption mitigation scheme.


2018 ◽  
Vol 136 ◽  
pp. 29-33 ◽  
Author(s):  
S. Pestchanyi ◽  
M. Lehnen ◽  
R.A. Pitts ◽  
G. Saibene

2021 ◽  
Author(s):  
Eric Nardon ◽  
Akinobu Matsuyama ◽  
Di Hu ◽  
Fabian Wieschollek

Abstract The possibility of using shattered pellet injection after the thermal quench of an ITER disruption in order to deplete Runaway Electron (RE) seeds before they can substantially avalanche is studied. Analytical and numerical estimates of the required injection rate for shards to be able to penetrate into the forming RE beam and stop REs are given. How much material could be assimilated before the Current Quench (CQ) becomes too short is also estimated. It appears that, if hydrogen pellets were used, the required number of pellets to be injected during the CQ would be prohibitive, at least considering the present design of the ITER Disruption Mitigation System (DMS). For neon or argon, the required number of pellets, although large, might be within reach of the ITER DMS, but the assimilated fraction would have to be very small in order not to shorten the CQ excessively. This study suggests that other injection schemes, based for example on small tungsten pellets coated with a low Z material, may be worth exploring as an option for an upgrade of the ITER DMS.


2021 ◽  
Author(s):  
Trey E Gebhart ◽  
Larry R Baylor ◽  
M Nance Ericson ◽  
Steve J Meitner ◽  
A Lou Qualls ◽  
...  

2012 ◽  
Vol 132 (7) ◽  
pp. 468-471
Author(s):  
Roger Raman ◽  
Daren P. Stotler ◽  
Tyler Abrams ◽  
Stephan P. Gerhardt ◽  
Thomas R. Jarboe ◽  
...  

2021 ◽  
Vol 164 ◽  
pp. 112200
Author(s):  
SooHwan Park ◽  
KunSu Lee ◽  
HyunMyung Lee ◽  
JaeIn Song ◽  
SangWon Yun ◽  
...  

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