Spatio-temporal evolution of the H → L back transition
Since ITER will operate close to threshold and with limited control, the H → L back transition is a topic important for machine operations as well as physics. Using a reduced mesoscale model [Miki et al., Phys. Plasmas 19, 092306 (2012)], we investigate ELM-free H → L back transition dynamics in ord...
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Veröffentlicht in: | Physics of plasmas 2013-06, Vol.20 (6) |
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Hauptverfasser: | , , , , , , |
Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | Since ITER will operate close to threshold and with limited control, the H → L back transition is a topic important for machine operations as well as physics. Using a reduced mesoscale model [Miki et al., Phys. Plasmas 19, 092306 (2012)], we investigate ELM-free H → L back transition dynamics in order to isolate transport physics effects. Model studies indicate that turbulence spreading is the key process which triggers the back transition. The transition involves a feedback loop linking turbulence and profiles. The I-phase appears during the back transition following a slow power ramp down, while fast ramp-downs reveal a single burst of zonal flow during the back transition. The I-phase nucleates at the pedestal shoulder, as this is the site of the residual turbulence in H-mode. Hysteresis in the profile gradient scale length is characterized by the Nusselt number, where
Nu
=
χ
i
,
turb
/
χ
i
,
neo
. Relative hysteresis of temperature gradient vs density gradient is sensitive to the pedestal Prandtl number, where
Pr
ped
=
D
ped
/
χ
i
,
neo
. We expect the H-mode to be somewhat more resilient in density than in temperature. |
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ISSN: | 1070-664X 1089-7674 |
DOI: | 10.1063/1.4812555 |