TY - JOUR
T1 - Predictive transport modelling and MHD stability analysis of mixed type I-II ELMy H-mode JET plasmas
AU - Lönnroth, J.-S.
AU - Parail, V.
AU - Huysmans, G.T.A.
AU - Saibene, G.
AU - Wilson, H.
AU - Sharapov, S.
AU - Corrigan, G.
AU - Heading, D.
AU - Sartori, R.
AU - Bécoulet, M.
AU - contributors, JET-EFDA
PY - 2004/5/1
Y1 - 2004/5/1
N2 - Mixed type I-II ELMy H-mode, a mode operation with small, frequent type
II edge localized modes (ELMs) interrupted by occasional large type I
ELMs, has been observed in various experimental situations. This paper
combines two simple models for type I and type II ELMs, respectively
(used e.g. in Lönnroth et al 2003 Plasma Phys. Control. Fusion 45
1689) into an improved scheme for modelling of mixed type I-II ELMy
H-mode, which has been implemented in the 1.5D core transport code JETTO
together with simple schemes for modelling of pure type I and type II
ELMy H-modes based on the same ideas. In the ELM modelling, transport
during the ELMs is enhanced by edge-localized radially Gaussian-shaped
perturbations to the transport coefficients. Type I and type II ELMs are
represented by perturbations with different widths and amplitudes and
controlled by different stability limits derived from
magnetohydrodynamic (MHD) stability analysis. Some justification from
theory and numerical analysis is given for the representation of each
ELM type. Predictive transport simulations with JETTO demonstrate that
the experimental dynamics of mixed type I-II ELMy H-mode can be
qualitatively reproduced using the present model. For completeness, the
modelling of mixed type I-II ELMy H-mode is compared with reference
simulations of pure type I and pure type II ELMy H-mode and the
differences, e.g. in confinement are explained. In addition, this paper
presents the results of MHD stability analysis of a number of situations
experimentally found to be favourable for the occurrence of type II
ELMs, namely situations with strong external neutral gas puffing, a
quasi-double-null magnetic configuration, high poloidal bgr (ratio of
the total pressure to the kinetic pressure) and combinations of high
edge safety factor q95 and high triangularity dgr. The
results of the analysis of the given scenarios are such that the model
used in this paper can explain why these situations can be favourable
for mixed type I-II or pure type II ELMy H-mode.
AB - Mixed type I-II ELMy H-mode, a mode operation with small, frequent type
II edge localized modes (ELMs) interrupted by occasional large type I
ELMs, has been observed in various experimental situations. This paper
combines two simple models for type I and type II ELMs, respectively
(used e.g. in Lönnroth et al 2003 Plasma Phys. Control. Fusion 45
1689) into an improved scheme for modelling of mixed type I-II ELMy
H-mode, which has been implemented in the 1.5D core transport code JETTO
together with simple schemes for modelling of pure type I and type II
ELMy H-modes based on the same ideas. In the ELM modelling, transport
during the ELMs is enhanced by edge-localized radially Gaussian-shaped
perturbations to the transport coefficients. Type I and type II ELMs are
represented by perturbations with different widths and amplitudes and
controlled by different stability limits derived from
magnetohydrodynamic (MHD) stability analysis. Some justification from
theory and numerical analysis is given for the representation of each
ELM type. Predictive transport simulations with JETTO demonstrate that
the experimental dynamics of mixed type I-II ELMy H-mode can be
qualitatively reproduced using the present model. For completeness, the
modelling of mixed type I-II ELMy H-mode is compared with reference
simulations of pure type I and pure type II ELMy H-mode and the
differences, e.g. in confinement are explained. In addition, this paper
presents the results of MHD stability analysis of a number of situations
experimentally found to be favourable for the occurrence of type II
ELMs, namely situations with strong external neutral gas puffing, a
quasi-double-null magnetic configuration, high poloidal bgr (ratio of
the total pressure to the kinetic pressure) and combinations of high
edge safety factor q95 and high triangularity dgr. The
results of the analysis of the given scenarios are such that the model
used in this paper can explain why these situations can be favourable
for mixed type I-II or pure type II ELMy H-mode.
U2 - 10.1088/0741-3335/46/5/004
DO - 10.1088/0741-3335/46/5/004
M3 - Article
SN - 0741-3335
VL - 46
SP - 767
EP - 796
JO - Plasma Physics and Controlled Fusion
JF - Plasma Physics and Controlled Fusion
IS - 5
ER -