Pedestal parametric scans to test ELM stability and evolution with new multifield fluctuation measurements
2024 Research Campaign, Pedestal and Non/Small ELM Regimes
Purpose of Experiment
This proposal aims at validating theoretical predictions of Edge-Localized-Mode (ELM) crashes, which are when the plasma edge expels a large burst of heat and particles, lowering the built-up pressure. It is thought that these occur due to an imbalance of stabilizing and destabilizing effects, such as the pressure gradient (how fast the pressure decreases as you move outwards in the plasma) and the edge current density (how much electrical current is flowing through the plasma) near the edge, as well as the plasma rotation (how fast the plasma spins). We aim to measure the current and rotation at ELM-relevant speeds with a new diagnostic built specifically for this, while also characterizing the plasma profiles and turbulent modes in-between ELM crashes. This will provide a valuable comparison that computational physicists can use to check the accuracy of their simulations when trying to model ELMs in other experiments or devices.
Experimental Approach
To study the ELM and turbulence characteristics, we will adjust collisionality, torque, and triangularity. These modifications will have a direct impact on the pedestal height and dynamics, turbulence drive, bootstrap current formation, and the rotation stabilization of the pedestal’s MHD and turbulent characteristics.
The rough shot design involves generating a stable version of shot 187219 (with the previously described modifications) and doing a minor current sweep to calibrate. Next, we will attempt a higher-power H-mode, during which co-current beams are replace by counter current beams halfway through the shot to obtain a scan in torque while keeping the total heating power constant. This initial shot will be repeated 1-2 times to obtain a spatial scan via the BES motorized fiber array. A full-field Bt=2.15T may be attempted next. Then, a series of shots with reducing triangularity will be performed, still with the beam-swap. Finally, we will reset to high-triangularity and increase density via puffing until we reach an analog of shot 196494 (but in Deuterium, with higher field/current). If time permits, we will finally reduce the field and current to attempt to mimic 196494 and obtain an accurate isotope comparison.