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Improved performance of ELMy H-modes at high density by plasma shaping in JET
144
Citations
26
References
2002
Year
EngineeringPlasma ShapingPlasma SciencePlasma PhysicsPlasma ConfigurationMagnetic Confinement FusionPlasma ThermalHigh DensityPlasma ShapeDivertor PhysicsPlasma TheoryPlasma SimulationPlasma ConfinementHigh Energy Density PhysicsPhysicsApplied Plasma PhysicFundamental Plasma PhysicMagnetic ConfinementNuclear AstrophysicsAerospace EngineeringNatural SciencesApplied PhysicsElmy H-modesPlasma Application
The study investigates how plasma shaping influences high‑density ELMy H‑mode performance in JET, using a magnetic boundary geometry relevant to ITER’s Q = 10 design. The experiments employed single lower‑null plasmas with standard q profiles, neutral‑beam heating, gas fuelling, and triangularity δ≈0.45–0.5 and elongation κ≈1.75. The results confirm that higher triangularity improves confinement and permits higher steady‑state densities, achieving up to 1.1 nGR (≈95 % nGR) at 2.5 MA/2.7 T with H98≈1 and βN≈2, while the stored thermal energy remains roughly constant with increasing density under Type I ELMs.
We present the results of experiments in JET to study the effect of plasma shape on high density ELMy H-modes, with geometry of the magnetic boundary similar to that envisaged for the standard Q = 10 operation in ITER. The experiments described are single lower null plasmas, with standard q profile, neutral beam heating and gas fuelling, with average plasma triangularity δ calculated at the separatrix ~0.45-0.5 and elongation κ~1.75. In agreement with the previous results obtained in JET and other divertor Tokamaks, the thermal energy confinement time and the maximum density achievable in steady state for a given confinement enhancement factor increase with δ. The new experiments have confirmed and extended the earlier results, achieving a maximum line average density ne~1.1nGR for H98~0.96. In this plasma configuration, at 2.5 MA/2.7 T (q95~2.8), a line average density ~95% nGR with H98 = 1 and βN~2 are obtained, with plasma thermal stored energy content Wth being approximately constant with increasing density, as long as the discharge maintains Type I ELMs, up to nped~nGR (and ne~1.1nGR).
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