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L-H transition in the mega-amp spherical tokamak
R J Akers1, G F Counsell, A Sykes
1EURATOM/UKAEA Fusion Association, Culham Science Centre, Abingdon, OXON, OX14 3DB, United Kingdom.
Physical Review Letters
|January 22, 2002
Summary
High-power H-mode plasmas were achieved on the MAST spherical tokamak, surpassing conventional predictions. This resulted in significantly improved energy confinement, even near density limits, with notable changes in plasma edge characteristics.
Area of Science:
- Plasma physics
- Fusion energy research
- Magnetic confinement fusion
Background:
- High-mode (H-mode) plasma confinement is crucial for achieving sustained fusion reactions.
- Conventional threshold scalings often underestimate the power required for H-mode transitions.
- The Mega Ampere Spherical Tokamak (MAST) is a key facility for studying tokamak physics.
Purpose of the Study:
- To investigate the achievement of H-mode plasmas in the MAST spherical tokamak at high input power.
- To analyze the energy confinement properties and plasma edge dynamics following the L-H transition.
- To compare experimental results with existing international scaling laws.
Main Methods:
- Operation of the MAST spherical tokamak.
- High-power plasma heating and fueling.
- Diagnostic measurements of plasma parameters, including density, temperature, turbulence, and rotation.
Main Results:
- H-mode plasmas were successfully achieved at input power significantly exceeding conventional threshold predictions.
- A substantial improvement in energy confinement was observed post-transition, outperforming international scalings.
- The transition was characterized by increased edge-density gradients, reduced turbulence, efficient wave conversion, and edge poloidal rotation.
Conclusions:
- The MAST spherical tokamak can achieve H-mode plasmas under conditions not predicted by standard scalings.
- The observed energy confinement improvements highlight the potential for enhanced performance in spherical tokamaks.
- The study provides valuable insights into the physics of the L-H transition and edge plasma dynamics.