Resistive Wall Tearing Mode Disruptions
ORAL
Abstract
Recent simulations of JET [1], ITER [2], DIII-D [3]
and Madison Symmetric Torus (MST) [4] found the thermal quench (TQ)
in disruptions was
caused by resistive wall tearing modes (RWTM).
In JET and DIII-D, with resistive wall time of 5ms,
the TQ time was found in simulations to be 1.5 ms and 2.5 ms respectively, in agreement
with experiment.
In ITER, with resistive wall time 250ms, simulations predict a TQ time of
about 100 ms. In MST
disruptions are not observed within the
the experimental shot time of 50ms.
Recent simulations and theory [4] found a TQ time of about 200 ms.
A model is presented of locked mode disruption precursors.
Impurity radiation and tearing mode island overlap cool the
edge and cause the current to contract. Model sequences of equilibria
with current contraction are analyzed for linear stability [5]. Current contraction
is found to destabilize RWTMs, while too much contraction stabilizes them.
This is consistent with DIII-D data, in which there is a minimum rational surface in which there is a minimum rational surface
radius for disruptions [4].
Active stabilization of RWTMs by feedback is under investigation with theory
and simulations. Results will be presented.
[1] H. Strauss and JET Contributors,
Phys. Plasmas 28, 032501 (2021)
[2] H. Strauss,
Phys. Plasmas 28 072507 (2021)
[3] H. Strauss, B. C. Lyons, M. Knolker,
Phys. Plasmas 29 112508 (2022).
[4] H. R. Strauss, B. E. Chapman, N. C. Hurst,
PPCF 65 084002 (2023).
[5] H. R. Strauss, arXiv (2023).
and Madison Symmetric Torus (MST) [4] found the thermal quench (TQ)
in disruptions was
caused by resistive wall tearing modes (RWTM).
In JET and DIII-D, with resistive wall time of 5ms,
the TQ time was found in simulations to be 1.5 ms and 2.5 ms respectively, in agreement
with experiment.
In ITER, with resistive wall time 250ms, simulations predict a TQ time of
about 100 ms. In MST
disruptions are not observed within the
the experimental shot time of 50ms.
Recent simulations and theory [4] found a TQ time of about 200 ms.
A model is presented of locked mode disruption precursors.
Impurity radiation and tearing mode island overlap cool the
edge and cause the current to contract. Model sequences of equilibria
with current contraction are analyzed for linear stability [5]. Current contraction
is found to destabilize RWTMs, while too much contraction stabilizes them.
This is consistent with DIII-D data, in which there is a minimum rational surface in which there is a minimum rational surface
radius for disruptions [4].
Active stabilization of RWTMs by feedback is under investigation with theory
and simulations. Results will be presented.
[1] H. Strauss and JET Contributors,
Phys. Plasmas 28, 032501 (2021)
[2] H. Strauss,
Phys. Plasmas 28 072507 (2021)
[3] H. Strauss, B. C. Lyons, M. Knolker,
Phys. Plasmas 29 112508 (2022).
[4] H. R. Strauss, B. E. Chapman, N. C. Hurst,
PPCF 65 084002 (2023).
[5] H. R. Strauss, arXiv (2023).
–
Publication: [1] H. Strauss and JET Contributors, <br>Phys. Plasmas 28, 032501 (2021) <br><br>[2] H. Strauss,<br> Phys. Plasmas 28 072507 (2021)<br><br>[3] H. Strauss, B. C. Lyons, M. Knolker,<br>Phys. Plasmas 29 112508 (2022).<br><br>[4] H. R. Strauss, B. E. Chapman, N. C. Hurst,<br>PPCF 65 084002 (2023).<br><br>[5] H. R. Strauss, arXiv (2023).
Presenters
-
Henry R Strauss
HRS Fusion
Authors
-
Henry R Strauss
HRS Fusion