2002
DOI: 10.1088/0029-5515/42/2/303
|View full text |Cite
|
Sign up to set email alerts
|

Shape dependence of sawtooth inversion radii and profile peaking factors in TCV L mode plasmas

Abstract: Sawtooth inversion radii and profile peaking factors of a large variety of ohmic and ECH heated L mode plasmas, including elongations up to 2.6 and triangularities between −0.5 and 0.75, have been investigated in the TCV tokamak. In ohmic plasmas, normalized inversion radii and electron temperature profile peaking factors (corrected for sawtoothing effects) depend solely on the parameter j /q 0 j 0 , irrespective of plasma shape. With ECH this parameter remains the main scaling parameter. Density profiles are … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

3
14
1

Year Published

2005
2005
2015
2015

Publication Types

Select...
10

Relationship

3
7

Authors

Journals

citations
Cited by 33 publications
(18 citation statements)
references
References 45 publications
3
14
1
Order By: Relevance
“…This convective mechanism, which is today often called "curvature" pinch [40,41], is predicted to increase the peaking of the density profile with increasing magnetic shear (or increasing peaking of the current density profile). This predicted dependence has been observed in data bases from several experiments, (TFTR [39], DIII-D [42,43], TCV [44], and JET [45]), and investigated in dedicated experiments in Tore Supra (TS) [46] and FTU [47]. However it appeared also clear that this dependence alone was not able to describe all the behaviors of the density profiles which were observed in tokamaks, because, in other conditions (and particularly in typical H-mode plasmas) this dependence was not observed [48,49].…”
Section: Considerations On the Validationsupporting
confidence: 71%
“…This convective mechanism, which is today often called "curvature" pinch [40,41], is predicted to increase the peaking of the density profile with increasing magnetic shear (or increasing peaking of the current density profile). This predicted dependence has been observed in data bases from several experiments, (TFTR [39], DIII-D [42,43], TCV [44], and JET [45]), and investigated in dedicated experiments in Tore Supra (TS) [46] and FTU [47]. However it appeared also clear that this dependence alone was not able to describe all the behaviors of the density profiles which were observed in tokamaks, because, in other conditions (and particularly in typical H-mode plasmas) this dependence was not observed [48,49].…”
Section: Considerations On the Validationsupporting
confidence: 71%
“…The peaking of the density profiles in these plasmas is in contrast with the flattening that is often observed in plasmas with central electron heating [37,38,39,40]. However, a detailed analysis of the electron and boron particle transport at mid-radius in these plasmas show that the experimental behaviors are well described by the theoretical modeling [41].…”
Section: Plasma Response To Ecrh Powermentioning
confidence: 99%
“…In figure 7(a) we compile the stationary normalized density gradients versus −ω QL R , such that the transition from a TEM to an ITG dominated regime is read from left to right, for theν − scan (open symbols: pentagrams, hexagrams, squares, crosses). We also add points from two additional s −ν scans performed at R/L Te = [10,12], R/L Ti = [6,7] to put in evidence the dependencies in the TEM branch (smaller open symbols: left triangles, up triangles, stars).…”
Section: Addressing the Experimental Observationsmentioning
confidence: 99%