intermediate phase
Recently Published Documents


TOTAL DOCUMENTS

958
(FIVE YEARS 225)

H-INDEX

54
(FIVE YEARS 9)

2021 ◽  
Author(s):  
Liang Chen ◽  
Guo Sheng Xu ◽  
Linming Shao ◽  
Wei Gao ◽  
Yifeng Wang ◽  
...  

Abstract In this paper, a comparison of dynamical features between the fast H-L and the H-I-L transition, which can be identified by the intermediate phase, or ‘I-phase’, has been made for radio-frequency (RF) heated deuterium plasmas in EAST. The fast H-L transition is characterized by a rapid release of stored energy during the transition transient, while the H-I-L transition exhibits a ‘soft’ H-mode termination. One important distinction between the transitions has been observed by dedicated probe measurements slightly inside the separatrix, with respect to the radial gradient of the floating potential, which corresponds to the E×B flow and/or the electron temperature gradient. The potential gradient inside the separatrix oscillates and persists during the stationary I-phase, and shows a larger amplitude than that before the fast H-L transition. The reduction of the gradient leads to the final transition to the L-mode for both the fast H-L and the H-I-L transition. These findings indicate that the mean E×B flow shear and/or edge electron temperature gradient play a critical role underlying the H-L transition physics. In addition, the back transition in EAST is found to be sensitive to magnetic configuration, where the vertical configuration, i.e., inner strike-point located at vertical target, favours access to the H-I-L transition, while the horizontal shape facilitates achievement of the fast H-L transition. The divertor recycling level normalized to electron density is higher before the fast H-L transition, as compared to that before the I-phase, which strongly suggest that the density of the recycled neutrals is an important ingredient in determining the back transition behaviour.


Author(s):  
Tat Loon Chng ◽  
David Z. Pai ◽  
Olivier Guaitella ◽  
Svetlana M Starikovskaia ◽  
Anne Bourdon

Abstract Electric field induced second harmonic (E-FISH) generation has emerged as a versatile tool for measuring absolute electric field strengths in time-varying, non-equilibrium plasmas and gas discharges. Yet recent work has demonstrated that the E-FISH signal, when produced with tightly focused laser beams, exhibits a strong dependence on both the length and shape of the applied electric field profile (along the axis of laser beam propagation). In this paper, we examine the effect of this dependence more meaningfully, by predicting what an E-FISH experiment would measure in a plasma, using 2D axisymmetric numerical fluid simulations as the true value. A pin-plane nanosecond discharge at atmospheric pressure is adopted as the test configuration, and the electric field evolution during the propagation of the ionization wave (IW) is specifically analyzed. We find that the various phases of this evolution (before and up to the front arrival, immediately behind the front and after the connection to the grounded plane) are quite accurately described by three unique electric field profile shapes, each of which produces a different response in the E-FISH signal. As a result, the accuracy of an E-FISH measurement is generally predicted to be comparable in the first and third phases of the IW evolution, and significantly poorer in the second (intermediate) phase. Fortunately, even though the absolute error in the field strength at certain time instants could be large, the overall shape of the field evolution curve is relatively well captured by E-FISH. Guided by the simulation results, we propose a procedure for estimating the error in the initial phase of the IW development, based on the presumption that the starting field profile mirrors that of its corresponding Laplacian conditions before evolving further. We expect that this approach may be readily generalized and applicable to other IW problems or phenomena, thus extending the utility of the E-FISH diagnostic.


2021 ◽  
pp. 2103019
Author(s):  
Shaomin Yang ◽  
Jialun Wen ◽  
Zhike Liu ◽  
Yuhang Che ◽  
Jie Xu ◽  
...  

Author(s):  
Jagannatha K B ◽  
B. Tanujit ◽  
Diptoshi Roy ◽  
S. Asokan ◽  
Chandasree Das

Joule ◽  
2021 ◽  
Author(s):  
Wanchun Xiang ◽  
Jiahuan Zhang ◽  
Shengzhong (Frank) Liu ◽  
Steve Albrecht ◽  
Anders Hagfeldt ◽  
...  

2021 ◽  
Vol 14 (3) ◽  
Author(s):  
José María Salvador-Gonzalez

St. Bonaventure asserts that man can ascend contemplatively to God through three phases. The first one is to contemplate God outside us by appreciating the corporeal things as vestiges of the deity: this is the “immanent” phase of Bonaventure’s Aesthetics, framed by the first and second stages of contemplation of God. The second phase consists of entering into our soul, as a spiritual image of God: this intermediate phase, in which we can contemplate God inside ourselves by his image in our soul, constitutes the Seraphic’s “introspective” Aesthetics, with the third and fourth stages of contemplation of God. In the third phase, man, transcending the vestiges in objects and the image of the deity in his soul, elevates himself to God, contemplating him as the spiritual and eternal First Principle: that third phase constitutes the Bonaventure’s “transcendent” Aesthetics, in which man can contemplate God considering his essential attributes (fifth stage) and his personal properties (sixth stage). The current article aims to highlight this fifth stage of Bonaventure’s Aesthetics. To achieve this goal, we analyze step by step the reasoning that, to prove his thesis, our author exposes in Chapter 5 of his Itinerarium mentis in Deum.


Sign in / Sign up

Export Citation Format

Share Document