Electron escape from negatively charged vortex rings incident on the free surface of He II

1972 ◽  
Vol 42 (3) ◽  
pp. 267-268 ◽  
Author(s):  
R.P. Mitchell ◽  
G.W. Rayfield
1997 ◽  
Vol 13 (2) ◽  
pp. 120-129 ◽  
Author(s):  
Ye Quyuan ◽  
C. K. Chu

1989 ◽  
Vol 1 (12) ◽  
pp. 2001-2004 ◽  
Author(s):  
L. P. Bernal ◽  
A. Hirsa ◽  
J. T. Kwon ◽  
W. W. Willmarth

2020 ◽  
Author(s):  
Abhay Kumar ◽  
Ashish Karn

The interaction of a submerged shallow synthetic jet with a parallel free surface has gathered substantial interest, owing to its relevance to the operation of marine vehicles viz. ships that move close to the water surface. However, despite exhaustive research on the perturbation on a free surface, very few studies have experimentally investigated the effect of unconfined water surface height on the evolution and propagation of a submerged synthetic jet. This study experimentally investigates a synthetic jet submerged in a quiescent flow at shallow depths ejecting parallel to the free surface, through qualitative analysis and quantitative measurements. The qualitative study includes the visualization of the flow using Plane Laser Induced Fluorescence (PLIF) technique, whereas the velocity measurements are carried out by a five-beam Laser Doppler Velocimetry (LDV) probe. The primary objective of these analysis and measurements is to gain a physical insight into the characteristics of vortex ring in a synthetic jet ejected from a fixed orifice at different water depths and at varying Reynolds number. Our studies indicate that the behavior of the vortex rings drastically changes as the depth of the jet crosses a certain threshold. Although no significant change in the path of synthetic jet is observed beyond a threshold depth in our experiments, the jet trajectory shows an interesting dependence on the Reynolds number based on circulation for shallow water depths. It has been found that in the shallow depths, the vortex ring drifts upwards and interacts with the free surface at lower Reynolds number, whereas for larger Reynolds number, the vortex ring rebounds near the free surface and moves downward. Based on our observations, it can be concluded that the phenomenon of upward/downward flection of vortex rings depends both upon its circulation and water depth.


2003 ◽  
Vol 2003 (0) ◽  
pp. 81
Author(s):  
Yuji Fukaya ◽  
Taiichi Nagata ◽  
Shinnosuke Obi ◽  
Shigeaki Masuda

1995 ◽  
Vol 117 (3) ◽  
pp. 374-381 ◽  
Author(s):  
A. Weigand ◽  
M. Gharib

The interaction of turbulent vortex rings that approach a clean water surface under various angles is experimentally investigated. The temporal evolution of the vortex rings with an initial Reynolds number of Re0 = 7500 is characterized by the laminar/turbulent transition and asymptotic relaminarization of the flow. Using the shadowgraph technique, two major flow cases were identified as a result of the vortex-ring/free-surface interaction: a trifurcation case that results from the interaction during the transition stage, and a bifurcation case that evolves during the fully-developed turbulent stage. In contrast to the laminar interaction, the turbulent bifurcation pattern is characterized by the reconnection and mutual interaction of many small-scale structures. Simultaneous digital particle image velocimetry (DPIV) and shadowgraph measurements reveal that the evolution of the small-scale structures at the free surface is strongly dominated by the bifurcation pattern, which in turn is a consequence of the persisting laminar sublayer in the core regions of the reconnected turbulent vortex loops.


1995 ◽  
Vol 11 (3) ◽  
pp. 229-238 ◽  
Author(s):  
Wu Chuijie ◽  
Fu Qiang ◽  
Ma Huiyang

2014 ◽  
Vol 65 ◽  
pp. 1-10 ◽  
Author(s):  
Naohisa Takagaki ◽  
Ryoichi Kurose ◽  
Yuya Baba ◽  
Yuichiro Nakajima ◽  
Satoru Komori
Keyword(s):  

Author(s):  
Jin Young Kim ◽  
R. E. Hummel ◽  
R. T. DeHoff

Gold thin film metallizations in microelectronic circuits have a distinct advantage over those consisting of aluminum because they are less susceptible to electromigration. When electromigration is no longer the principal failure mechanism, other failure mechanisms caused by d.c. stressing might become important. In gold thin-film metallizations, grain boundary grooving is the principal failure mechanism.Previous studies have shown that grain boundary grooving in gold films can be prevented by an indium underlay between the substrate and gold. The beneficial effect of the In/Au composite film is mainly due to roughening of the surface of the gold films, redistribution of indium on the gold films and formation of In2O3 on the free surface and along the grain boundaries of the gold films during air annealing.


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