scholarly journals Filaments in the edge confinement region of TJ-II

2018 ◽  
Vol 58 (2) ◽  
pp. 026030 ◽  
Author(s):  
B.Ph. van Milligen ◽  
J.H. Nicolau ◽  
B. Liu ◽  
G. Grenfell ◽  
U. Losada ◽  
...  
Keyword(s):  
2020 ◽  
Vol 10 (1) ◽  
Author(s):  
N. Kenmochi ◽  
T. Minami ◽  
T. Mizuuchi ◽  
C. Takahashi ◽  
G. M. Weir ◽  
...  

AbstractWhen realising future fusion reactors, their stationary burning must be maintained and the heat flux to the divertor must be reduced. This essentially requires a stationary internal transport barrier (ITB) plasma with a fast control system. However, the time scale for determining the position of the foot point of an ITB is not clearly understood even though its understanding is indispensable for fast profile control. In this study, the foot point of the electron ITB (eITB) was observed to be reformed at the vicinity of a magnetic island when the island started to form. In addition, the enhanced confinement region was observed to expand during the eITB formation according to the radial movement of the magnetic island toward the outer region. Compared to the time scales of the local heat transport, the faster time scales of the movement of the eITB foot point immediately after island formation (~0.5 ms) suggest the importance of the magnetic island for plasma profile control to maintain stationary burning.


2020 ◽  
Vol 22 (14) ◽  
pp. 7250-7258
Author(s):  
Guilherme Ribeiro Portugal ◽  
Jeverson Teodoro Arantes

Sodium tantalate 1-D nanostructures show novel properties due to their edge confinement region, which may be relevant for distinct applications.


1998 ◽  
Vol 120 (1) ◽  
pp. 68-72 ◽  
Author(s):  
G. K. Morris ◽  
S. V. Garimella

The flow fields in the orifice and the confinement region of a normally impinging, axisymmetric, confined, and submerged liquid jet were computationally investigated. Numerical predictions were made for orifice diameters of 3.18 and 6.35 mm at several orifice-to-target plate spacings, with turbulent jet Reynolds number ranging from 8500 to 23,000. The commercial finite-volume code FLUENT was used to solve the flow fields using a modified k–ε model based on renormalization group theory. The predicted characteristics of the separation region at the entrance of the orifice agree with experiments in the literature. The pressure drop across the orifice was predicted to within 5 percent of proposed empirical correlations based on published experimental data. The computed flow patterns in the confinement region of the impinging jet were in good qualitative agreement with flow visualizations; however, a secondary recirculation zone observed in experiments was not predicted by the models. The results presented for the flow (and pressure drop) in the orifice, as well as that in the confined outflow region, influence heat transfer on the impingement surface and are important considerations in electronics packaging design.


2014 ◽  
Vol 21 (11) ◽  
pp. 114502 ◽  
Author(s):  
Kiyoyuki Yambe ◽  
Yoichi Hirano ◽  
Hajime Sakakita ◽  
Haruhisa Koguchi

Author(s):  
И.Ю. Сениченков ◽  
Е.Г. Кавеева ◽  
В.А. Рожанский ◽  
Е.А. Сытова ◽  
И.Ю. Веселова ◽  
...  

AbstractModeling of the transition to the detachment of ASDEX Upgrade tokamak plasma with increasing density is performed using the SOLPS-ITER numerical code with a self-consistent account of drifts and currents. Their role in plasma redistribution both in the confinement region and in the scrape-off layer (SOL) is investigated. The mechanism of high field side high-density formation in the SOL in the course of detachment is suggested. In the full detachment regime, when the cold plasma region expands above the X -point and reaches closed magnetic-flux surfaces, plasma perturbation in a confined region may lead to a change in the confinement regime.


2019 ◽  
Vol 204 ◽  
pp. 01002
Author(s):  
Viatcheslav Kuvshinov ◽  
Valery Shaparau ◽  
Eugene Bagashov

It is shown that the interaction of quark with the stochastic vacuum of QCD (considered as an environment) leads to the decoherence of quark colour state, associated with the loss of information on the initial quark colour. We propose to consider this process as a reason of the confinement of the quark colour. Asymptotically this leads to confined quarks (fully mixed colourless quark states) in the limit of large distances and time intervals (confinement region) and free coloured quarks in the limit of small distances and time intervals (asymptotic freedom). We propose quantitative characteristics that allow to describe the process of interaction: purity, fidelity, von Neumann entropy, quantum information measure. The cases of two and arbitrary number of quarks are considered, and it is shown that the entanglement in such system disappears in the limit of large distances and time intervals. The process is in good agreement with the known theorems in quantum information theory (no-cloning and no-hiding). We study non-perturbative evolution of the gluon colour states during short time. Fluctuations of gluons are less than those for coherent states. This fact suggests that there gluon squeezed states can arise. Theoretical justification for the occurrence both singe- and two-mode gluon squeezing effects in QCD is given. We show that gluon entangled states which are closely related with two-mode squeezed states of gluon fields can appear at short time non-perturbative evolution by analogy with corresponding photon states in quantum optics.


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