Hot tail runaway electron generation in tokamak disruptions

2008 ◽  
Vol 15 (7) ◽  
pp. 072502 ◽  
Author(s):  
H. M. Smith ◽  
E. Verwichte
2015 ◽  
Vol 81 (5) ◽  
Author(s):  
A. Lvovskiy ◽  
H. R. Koslowski ◽  
L. Zeng ◽  

Disruptions with runaway electron generation have been deliberately induced by injection of argon using a disruption mitigation valve. A second disruption mitigation valve has been utilised to inject varying amounts of helium after a short time delay. No generation of runaway electrons has been observed when more than a critical amount of helium has been injected no later than 5 ms after the triggering of the first valve. The required amount of helium for suppression of runaway electron generation is up to one order of magnitude lower than the critical density according to Connor & Hastie (1975) and Rosenbluth & Putvinski (1997).


2020 ◽  
Vol 86 (4) ◽  
Author(s):  
K. Insulander Björk ◽  
G. Papp ◽  
O. Embreus ◽  
L. Hesslow ◽  
T. Fülöp ◽  
...  

Massive material injection has been proposed as a way to mitigate the formation of a beam of relativistic runaway electrons that may result from a disruption in tokamak plasmas. In this paper we analyse runaway generation observed in eleven ASDEX Upgrade discharges where disruption was triggered using massive gas injection. We present numerical simulations in scenarios characteristic of on-axis plasma conditions, constrained by experimental observations, using a description of the runaway dynamics with a self-consistent electric field and temperature evolution in two-dimensional momentum space and zero-dimensional real space. We describe the evolution of the electron distribution function during the disruption, and show that the runaway seed generation is dominated by hot-tail in all of the simulated discharges. We reproduce the observed dependence of the current dissipation rate on the amount of injected argon during the runaway plateau phase. Our simulations also indicate that above a threshold amount of injected argon, the current density after the current quench depends strongly on the argon densities. This trend is not observed in the experiments, which suggests that effects not captured by zero-dimensional kinetic modelling – such as runaway seed transport – are also important.


2020 ◽  
Vol 60 (8) ◽  
pp. 084002
Author(s):  
X. Zhu ◽  
L. Zeng ◽  
Y. Liang ◽  
S. Lin ◽  
Y. Liu ◽  
...  

2005 ◽  
Vol 12 (12) ◽  
pp. 122505 ◽  
Author(s):  
H. Smith ◽  
P. Helander ◽  
L.-G. Eriksson ◽  
T. Fülöp

2009 ◽  
Vol 51 (12) ◽  
pp. 124008 ◽  
Author(s):  
H M Smith ◽  
T Fehér ◽  
T Fülöp ◽  
K Gál ◽  
E Verwichte

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