Abstract. The well-known and potentially disruptive plasma “current rise” instabilities are studied as a function of the plasma shape in the tokamak à Configuration Variable (TCV). Disruptions typically occur in quasi-circular plasmas at qa ∼ 3 in both non-sawtoothing and sawtoothing discharges with peaked current profiles. The perturbations in the plasma parameters before disruption are characterised, and the main unstable modes identified as coupled m/n=2/1 and 3/2 rotating tearing modes. In the early phase, coupling between 3/1 and 2/1 modes is found to play a major role in determining whether or not the disruption will occur. Plasma cross section shaping is observed to reduce or to completely stabilise the disruptive mode and is regula...
Progress in the area of MHD stability and disruptions, since the publication of the 1999 ITER Physic...
Progress in the area of MHD stability and disruptions, since the publication of the 1999 ITER Physic...
Progress in the area of MHD stability and disruptions, since the publication of the 1999 ITER Physic...
The beneficial effect of plasma shaping during the initial current ramp up of L-mode ohmic discharge...
Magnetohydrodynamic (MHD) instabilities and plasma rotation have various impacts on particle and the...
In the TCV tokamak the sawtooth period and the sawtooth amplitude are observed to depend strongly on...
During the operation of the TCV tokamak an extremely wide variety of plasma shapes has been controll...
ABSTRACT. The energy confinement time of TCV ohmic L mode discharges depends strongly on plasma shap...
Low-m tearing modes constitute the dominant instability problem in present-day tokamaks. In this lec...
A large variety of plasma conditions has been created in TCV (Tokamak à Configura-tion Variable, BT&...
“Advanced tokamak” (AT) scenarios were developed with the aim of reaching steady-state operation in ...
MHD modes always occur in ASDEX Upgrade before q-limit and density limit disruptions. The modulation...
In cylindrical geometry, we analyze the hypothesis that the major disruption in tokamaks is due to t...
The purpose of this paper is to further investigate the major disruptions occurring in low-q(a) disc...
A general introduction to ideal magnetohydrodynamic (MHD) stability of tokamak plasmas is given, usi...
Progress in the area of MHD stability and disruptions, since the publication of the 1999 ITER Physic...
Progress in the area of MHD stability and disruptions, since the publication of the 1999 ITER Physic...
Progress in the area of MHD stability and disruptions, since the publication of the 1999 ITER Physic...
The beneficial effect of plasma shaping during the initial current ramp up of L-mode ohmic discharge...
Magnetohydrodynamic (MHD) instabilities and plasma rotation have various impacts on particle and the...
In the TCV tokamak the sawtooth period and the sawtooth amplitude are observed to depend strongly on...
During the operation of the TCV tokamak an extremely wide variety of plasma shapes has been controll...
ABSTRACT. The energy confinement time of TCV ohmic L mode discharges depends strongly on plasma shap...
Low-m tearing modes constitute the dominant instability problem in present-day tokamaks. In this lec...
A large variety of plasma conditions has been created in TCV (Tokamak à Configura-tion Variable, BT&...
“Advanced tokamak” (AT) scenarios were developed with the aim of reaching steady-state operation in ...
MHD modes always occur in ASDEX Upgrade before q-limit and density limit disruptions. The modulation...
In cylindrical geometry, we analyze the hypothesis that the major disruption in tokamaks is due to t...
The purpose of this paper is to further investigate the major disruptions occurring in low-q(a) disc...
A general introduction to ideal magnetohydrodynamic (MHD) stability of tokamak plasmas is given, usi...
Progress in the area of MHD stability and disruptions, since the publication of the 1999 ITER Physic...
Progress in the area of MHD stability and disruptions, since the publication of the 1999 ITER Physic...
Progress in the area of MHD stability and disruptions, since the publication of the 1999 ITER Physic...