H-mode profile parametrization for extrapolation and control

Imre, Kaya; Riedel, Kurt S.; Schissel, D.P.; Schunke, B.

doi:10.1088/0741-3335/38/8/058

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“…For JET, the L-mode confinement [9] tends to scale as τ E ∼ I .9 p B .5 t , which shows more of a B t dependence. Equation (8) indicates that the improvement in L-mode confinement time with increasing B pol /B t is not due to improved confinement of bulk electrons. Thus the I p dependence of the τ E scaling is associated with improved confinement of ions or fast particles or possibly due to a reduction in Z ef f and the corresponding increase in ion density.…”

Section: L-mode Temperaturementioning

confidence: 99%

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Profile shape parameterization of JET electron temperature and density profiles

Schunke

Imre²,

Riedel³

1997

Nucl. Fusion

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The temperature and density profiles of the Joint European Torus are parameterised using log-additive models in the control variables. Predictive error criteria are used to determine which terms in the log-linear model to include. The density and temperature profiles are normalised to their line averages (n and T ). The normalised Ohmic density shape depends primarily on the parameter n/B t , where B t is the toroidal magnetic field. Both the Low-mode (L-mode) and edge localized mode-free (ELM-free) high mode (H-mode) temperature profile shapes depend strongly on the type of heating power, with ion cyclotron resonant heating producing a more peaked profile than neutral beam injection. Given the heating type dependence, the L-mode temperature shape is nearly independent of the other control variables. The H-mode temperature shape broadens as the effective charge, Z ef f , increases. The line average L-mode temperature scales as B .96 t (Power per particle) .385 . The L-mode normalised density shape depends primarily on the ratio of line average density, n, to the edge safety factor, q 95 . As n/q 95 increases, the profile shape broadens. The current, I p , is the most important control variable for the normalised Hmode density. As the current increases, the profile broadens and the gradient at the edge sharpens. Increasing the heating power, especially the ion cyclotron resonant heating, or decreasing the average density, peaks the H-mode density profile slightly.

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Section: L-mode Temperaturementioning

confidence: 99%

“…To determine the size dependence and examine intra-machine variability, a multi-machine database with an expanded parameter space is necessary. Work on a combined DIII-D-JET profile parameterisation has begun [7,8] .…”

Section: Introductionmentioning

confidence: 99%