4th Transport/ITB IPTA Meeting, St Petersburg, 8-12 April 2003 1 Role of Edge Current in ELM Behaviour: Modelling of Recent Current Ramp Experiment in JET V.V. Parail 1 , G. Bateman 6 , M. Becoulet 4 , G. Corrigan 1 , A.Y. Dnestrovskij 2 , G. Huysmans 4 , A. Kritz 6 , A. Loarte 5 , J. Lonnroth 3 , T. Onjun 6 , G. Saibene 5 , H. Wilson 1 1 UKAEA Fusion Association, Culham, UK; 2 Kurchatov Institute, Moscow, Russia, 3 Association Euratom-Tekes, Finland; 4 Association Euratom-CEA, Cadarache, France; 5 EFDA-CSU, Garching, Germany, 6 Lehigh Univ., PA • Peeling vs. ballooning stability; • Recent current ramp-up experiments; • Predictive modelling of JET ELMy H-mode plasmas; • Conclusions and future plans
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Role of Edge Current in ELM Behaviour: Modelling of Recent Current Ramp Experiment in JET
Role of Edge Current in ELM Behaviour: Modelling of Recent Current Ramp Experiment in JET. V.V. Parail 1 , G. Bateman 6 , M. Becoulet 4 , G. Corrigan 1 , A.Y. Dnestrovskij 2 , G. Huysmans 4 , A. Kritz 6 , A. Loarte 5 , J. Lonnroth 3 , T. Onjun 6 , G. Saibene 5 , H. Wilson 1 - PowerPoint PPT Presentation
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4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 1
Role of Edge Current in ELM Behaviour: Modelling of Recent Current Ramp
Experiment in JETV.V. Parail1, G. Bateman6, M. Becoulet4, G. Corrigan1, A.Y.
Dnestrovskij2, G. Huysmans4, A. Kritz6, A. Loarte5, J. Lonnroth3, T. Onjun6, G. Saibene5 , H. Wilson1
• Peeling vs. ballooning stability;• Recent current ramp-up experiments;• Predictive modelling of JET ELMy H-mode plasmas;• Conclusions and future plans
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 2
Current ramp-up experiment on JETBtor=3.4T
Ip=2MA
=0.4
=1.7
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 3
Peeling vs. ballooning stability (1) We adopt the following approach in predictive
modelling :
we assume certain width of the ETB (either constant or dependent on plasma parameters);
we simulate all main plasma profiles (ne, Te,i, jII, + neutrals) up to and beyond the separatrix by using a coupling of two codes: JETTO+EDGE2D;
we can make different assumptions about ELM trigger (ideal ballooning with and without access to a second stability, peeling mode);
we use ad hoc model for ELM amplitude and duration
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 4
Peeling vs. ballooning stability (2)
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 5
Peeling vs. ballooning stability (3)
0
0.02
0.04
0.06
0.08
0.1
0 1 2 3
Stable
Unstable
J ed
ge/J
avge
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 6
Peeling vs. ballooning stability (4)
Simple analytical criteria for ballooning and peeling mode stability are used in JETTO as an ELM trigger:
Ballooning mode: with
adjustable parameter to account for an access to a second stability region;
Peeling mode:
critp
200
ddp
Br2
0
crit
dlBR
Bjq22
1D41 3p
2II
M '
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 7
Peeling vs. ballooning stability (5)
We can use either one or both criteria in our predictive modelling;
the caveat is that ELM-event itself is independent on the ELM trigger - it appears as a short sharp increase in heat and particle diffusivities (but not in electrical resistivity) within the ETB;
it means that ELM quickly destroys the edge bootstrap current but it takes much longer to dissipate the Ohmic current, which substitutes bootstrap current;
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 8
Peeling vs. ballooning stability (6)
We study the relative role of ballooning and peeling mode instability as ELM trigger in our predictive modelling;
In experiment the easiest way to decouple the edge current from the pressure gradient (bootstrap current) is to ramp the current during the ELMy H-mode;
JET recently conducted a dedicated experiment, in which current ramp-up technique was used in low density Optimised Shear plasmas;
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 9
Selection of shots (1)Btor=3.4T
Ip=2MA
=0.4
=1.7
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 10
Selection of shots (2)
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 11
Predictive Modelling of ELMs (1)First we demonstrate that we can reproduce
experimental data with ballooning stability trigger;
Ballooning stability trigger with
JET #53298
2crit
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 12
Predictive Modelling of ELMs (2)First we demonstrate that we can reproduce
experimental data with ballooning stability trigger;
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 13
Predictive Modelling of ELMs (3) Then we study the relative role of ballooning and
peeling mode as an ELM trigger;
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 14
Predictive Modelling of ELMs (4) Or with a better resolution:
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 15
Predictive Modelling of ELMs (5)
We conclude that both ballooning and peeling mode trigger ELM within the experimentally observed parameter range;
If peeling mode is used as ELM trigger the ELM duration becomes much longer than experimentally observed length telm<0.2msec;
The explanation is that the edge current should be removed in order to suppress peeling mode and this current is controlled by the skin time;
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 16
Predictive Modelling of ELMs (6)
We also found that ELM has a composite character in many cases: it is triggered by ballooning mode, which is superseded by the peeling mode:
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 17
Predictive Modelling of ELMs (7)
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 18
Predictive Modelling of ELMs (8) It is interesting to note that since skin time is
proportional to skinTe3/2, the ELM duration
should depend on edge temperature;
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 19
Predictive Modelling of ELMs (9) Now we can check how our combined peeling-
ballooning model for ELM trigger will react on the current ramp:
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 20
Predictive Modelling of ELMs (10) or, with a better resolution:
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 21
Predictive Modelling of ELMs (11) Qualitatively (only!) it goes in line with experiment:
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 22
Predictive Modelling of ELMs (12) Qualitatively (only!) it goes in line with experiment;
We can easily reproduce temperature and density profiles but not ELM dynamics;
4th Transport/ITB IPTA Meeting, St Petersburg,
8-12 April 2003 23
Conclusions
Experimental observations and predictive modelling show that both ballooning and peeling mode can play their part in ELMs;
Recent current ramp-up experiment in JET (although not quite conclusive) indicate that peeling mode might play a crucial role in keeping plasma edge in type-III ELMy H-mode in low density plasmas;