1999
DOI: 10.1103/physrevlett.82.5048
|View full text |Cite
|
Sign up to set email alerts
|

Nonlocal Transient Transport and Thermal Barriers in Rijnhuizen Tokamak Project Plasmas

Abstract: In the Rijnhuizen Tokamak Project plasmas, a transient rise of the core electron temperature is observed when hydrogen pellets are injected tangentially to induce fast cooling of the peripheral region. High-resolution Thomson scattering measurements show that the T e rise is associated with large temperature gradients in the region 1 , q , 2. This region acts as a layer of transiently increased thermal resistivity (transport barrier) when probed by fast heat pulses from modulated electron cyclotron heating.[S0… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

16
107
0
2

Year Published

2001
2001
2024
2024

Publication Types

Select...
8
1

Relationship

0
9

Authors

Journals

citations
Cited by 89 publications
(125 citation statements)
references
References 5 publications
16
107
0
2
Order By: Relevance
“…Following the edge cooling, there was a rapid increase of the core electron temperature, on a time scale (∼5 ms) faster than the diffusive time. This effect is suggestive of a short-lived internal transport barrier (ITB), triggered by the sudden increase of the edge temperature gradient, which can be modeled with an abrupt drop in the core electron thermal conductivity [19,20,21,23,24,25,27], and which persists for the duration of the edge cooling (∼30 ms). A model for this transient increase in electron heat transport (a drop in thermal conductivity) is shown in Fig.3, with a 25% drop in χ e near r/a = 0.3 (solid to dash-dot lines).…”
Section: Methodsmentioning
confidence: 99%
“…Following the edge cooling, there was a rapid increase of the core electron temperature, on a time scale (∼5 ms) faster than the diffusive time. This effect is suggestive of a short-lived internal transport barrier (ITB), triggered by the sudden increase of the edge temperature gradient, which can be modeled with an abrupt drop in the core electron thermal conductivity [19,20,21,23,24,25,27], and which persists for the duration of the edge cooling (∼30 ms). A model for this transient increase in electron heat transport (a drop in thermal conductivity) is shown in Fig.3, with a 25% drop in χ e near r/a = 0.3 (solid to dash-dot lines).…”
Section: Methodsmentioning
confidence: 99%
“…These facts have been emphasised both theoretically: through the description of avalanching and spreading, [3][4][5][6][7][8][9] through the characterisation of nonlocal, nondiffusive behaviour 1,[10][11][12] and experimentally through some yet-to-be-understood experimental jigsaws: deep inconsistencies with a (fixed gradient) local and diffusive modeling have indeed been reported in perturbative (either hot or cold pulse) experiments, [13][14][15][16][17] off-axis heating experiments, 19,20 or whilst reporting Bohm-like scalings of the energy confinement time. 18 An accurate description of such dynamics requires the simultaneous and self-consistent treatment of the full gyrokinetic distribution function (full-f modeling), in full-torus (global) tokamak geometry and for a prescribed distribution of sources and sinks (flux-driven description).…”
Section: Introductionmentioning
confidence: 99%
“…This effect is a key for understanding why "the tail wags the plasma," i.e., why jogging edge flows by changing magnetic geometry leaves a footprint in the core flow. A perturbative experiment [23][24][25][26][27][28] is proposed as a further critical test.…”
mentioning
confidence: 99%
“…Another important consequence that the nonlinear flux can induce is the dynamic response of the core flows against the edge perturbation [23][24][25][26][27][28]. As discussed above, the nonlinear flux allows the fluctuation momentum to propagate faster than the mean momentum.…”
mentioning
confidence: 99%