Behavior of n = 1 magnetohydrodynamic modes of infernal type at high-mode pedestal with plasma rotation

2013 ◽  
Vol 20 (1) ◽  
pp. 012501 ◽  
Author(s):  
L. J. Zheng ◽  
M. T. Kotschenreuther ◽  
P. Valanju
Keyword(s):  
High Mode ◽  
Plasma Rotation

scholarly journals Diamagnetic drift effects on the low-n magnetohydrodynamic modes at the high mode pedestal with plasma rotation

2014 ◽  
Vol 21 (6) ◽  
pp. 062502 ◽  
Author(s):  
L. J. Zheng ◽  
M. T. Kotschenreuther ◽  
P. Valanju
Keyword(s):  
High Mode ◽  
Plasma Rotation ◽  
Diamagnetic Drift

Effect on plasma rotation of lower hybrid (LH) waves in Alcator C-Mod

2014 ◽  
Author(s):  
J. P. Lee ◽  
M. Barnes ◽  
R. R. Parker ◽  
J. E. Rice ◽  
F. I. Parra ◽  
...  
Keyword(s):  
Lower Hybrid ◽  
Plasma Rotation

High-mode wave reliefs in a spatially nonlocal erosion model

2014 ◽  
Vol 43 (4) ◽  
pp. 277-283
Author(s):  
A. S. Rudyi ◽  
A. N. Kulikov ◽  
D. A. Kulikov ◽  
A. V. Metlitskaya
Keyword(s):  
High Mode ◽  
Erosion Model ◽  
Mode Wave

scholarly journals Correction factor determination on failure rate equation of MacLaurin series for low and high mode application

2016 ◽  
Vol 7 (2) ◽  
pp. 827-834
Author(s):  
Totok R. Biyanto ◽  
Franky Kusuma ◽  
Ali Musyafa ◽  
Ronny Dwi Noriyati ◽  
Ridho Bayuaji ◽  
...  
Keyword(s):  
Failure Rate ◽  
Correction Factor ◽  
Rate Equation ◽  
High Mode ◽  
Maclaurin Series

Heavy impurity transport in tokamaks subject to plasma rotation, NTV and the influence of saturated ideal MHD perturbations

2021 ◽  
Author(s):  
Eduardo Lascas Neto ◽  
Jonathan P Graves ◽  
Madhusudan Raghunathan ◽  
Cristian Sommariva ◽  
David Pfefferlé
Keyword(s):  
Magnetic Fields ◽  
Electric Field ◽  
High Performance ◽  
Plasma Rotation ◽  
Impurity Transport ◽  
Heavy Impurity ◽  
Outward Transport ◽  
Ideal Mhd ◽  
Plasma Configuration

Abstract Strongly peaked tungsten accumulation is a common feature of high performance plasma scenarios in JET with the ITER-like wall, particularly during MHD activity induced by m⁄n = 1⁄1 continuous modes. This study investigates the effect of 1⁄1 long living internal kink modes on heavy impurity transport in the presence of strong flows and NTV ambipolar electric field. A novel formulation which includes these effects is presented and applied in the VENUS-LEVIS code in order to follow tungsten ions in a saturated JET-like 1⁄1 internal kinked toroidally rotating plasma configuration. The synergy between 3D magnetic fields, strong flows and NTV is seen to cause tungsten accumulation in contrast to what is observed in similar axisymmetric configurations. Rapid inward transport of impurities in JET plasmas following the triggering of continuous 1⁄1 modes is explained by the work presented here, and we use the same theory to postulate why outward transport can occur in kinked ASDEX-U plasmas.

Plasma rotation in the PDX tokamak

1983 ◽  
Vol 23 (12) ◽  
pp. 1643-1655 ◽  
Author(s):  
K. Brau ◽  
M. Bitter ◽  
R.J. Goldston ◽  
D. Manos ◽  
K. McGuire ◽  
...  
Keyword(s):  
Plasma Rotation

Effect of Shortened Light-Curing Modes on Bulk-Fill Resin Composites

2020 ◽  
Vol 45 (5) ◽  
pp. 496-505
Author(s):  
CS Sampaio ◽  
PG Pizarro ◽  
PJ Atria ◽  
R Hirata ◽  
M Giannini ◽  
...  
Keyword(s):  
Tensile Strength ◽  
Bond Strength ◽  
Shear Bond Strength ◽  
Light Output ◽  
High Mode ◽  
Resin Composites ◽  
Curing Time ◽  
Micro Computed Tomography ◽  
Polymerization Shrinkage ◽  
Light Curing

Clinical Relevance Shortened light curing does not affect volumetric polymerization shrinkage or cohesive tensile strength but negatively affects the shear bond strength of some bulk-fill resin composites. When performing shortened light curing, clinicians should be aware of the light output of their light-curing units. SUMMARY Purpose: To evaluate volumetric polymerization shrinkage (VPS), shear bond strength (SBS) to dentin, and cohesive tensile strength (CTS) of bulk-fill resin composites (BFRCs) light activated by different modes. Methods and Materials: Six groups were evaluated: Tetric EvoCeram bulk fill + high mode (10 seconds; TEC H10), Tetric EvoFlow bulk fill + high mode (TEF H10), experimental bulk fill + high mode (TEE H10), Tetric EvoCeram bulk fill + turbo mode (five seconds; TEC T5), Tetric EvoFlow bulk fill + turbo mode (TEF T5), and experimental bulk fill + turbo mode (TEE T5). Bluephase Style 20i and Adhese Universal Vivapen were used for all groups. All BFRC samples were built up on human molar bur-prepared occlusal cavities. VPS% and location were evaluated through micro–computed tomography. SBS and CTS tests were performed 24 hours after storage or after 5000 thermal cycles; fracture mode was analyzed for SBS. Results: Both TEC H10 and TEE H10 presented lower VPS% than TEF H10. However, no significant differences were observed with the turbo-curing mode. No differences were observed for the same BFRC within curing modes. Occlusal shrinkage was mostly observed. Regarding SBS, thermal cycling (TC) affected all groups. Without TC, all groups showed higher SBS values for high mode than turbo mode, while with TC, only TEC showed decreased SBS from high mode to turbo modes; modes of fracture were predominantly adhesive. For CTS, TC affected all groups except TEE H10. In general, no differences were observed between groups when comparing the curing modes. Conclusions: Increased light output with a shortened curing time did not jeopardize the VPS and SBS properties of the BFRCs, although a decreased SBS was observed in some groups. TEE generally showed similar or improved values for the tested properties in a shortened light-curing time. The VPS was mostly affected by the materials tested, whereas the SBS was affected by the materials, curing modes, and TC. The CTS was not affected by the curing modes.

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