Single-vortex fluctuations in layered superconductors: Electromagnetic coupling and crossover to strong pinning

2004 ◽  
Vol 69 (14) ◽  
Author(s):  
Jan Kierfeld
1993 ◽  
Vol 70 (12) ◽  
pp. 1870-1873 ◽  
Author(s):  
V. G. Kogan ◽  
M. Ledvij ◽  
A. Yu. Simonov ◽  
J. H. Cho ◽  
D. C. Johnston

1996 ◽  
Vol 54 (1) ◽  
pp. 72-75 ◽  
Author(s):  
Gianni Blatter ◽  
Vadim Geshkenbein ◽  
Anatoli Larkin ◽  
Henrik Nordborg

1996 ◽  
Vol 53 (14) ◽  
pp. R8855-R8858 ◽  
Author(s):  
A. E. Koshelev ◽  
P. Le Doussal ◽  
V. M. Vinokur

1993 ◽  
Vol 48 (14) ◽  
pp. 10448-10456 ◽  
Author(s):  
G. Blatter ◽  
B. Ivlev ◽  
H. Nordborg

1999 ◽  
Vol 09 (PR10) ◽  
pp. Pr10-289-Pr10-291
Author(s):  
Yu. I. Latyshev ◽  
T. Yamashita

Author(s):  
Johan Roenby ◽  
Hassan Aref

The model of body–vortex interactions, where the fluid flow is planar, ideal and unbounded, and the vortex is a point vortex, is studied. The body may have a constant circulation around it. The governing equations for the general case of a freely moving body of arbitrary shape and mass density and an arbitrary number of point vortices are presented. The case of a body and a single vortex is then investigated numerically in detail. In this paper, the body is a homogeneous, elliptical cylinder. For large body–vortex separations, the system behaves much like a vortex pair regardless of body shape. The case of a circle is integrable. As the body is made slightly elliptic, a chaotic region grows from an unstable relative equilibrium of the circle-vortex case. The case of a cylindrical body of any shape moving in fluid otherwise at rest is also integrable. A second transition to chaos arises from the limit between rocking and tumbling motion of the body known in this case. In both instances, the chaos may be detected both in the body motion and in the vortex motion. The effect of increasing body mass at a fixed body shape is to damp the chaos.


Metals ◽  
2021 ◽  
Vol 11 (3) ◽  
pp. 398
Author(s):  
Jesus Gonzalez-Trejo ◽  
Cesar A. Real-Ramirez ◽  
Jose Raul Miranda-Tello ◽  
Ruslan Gabbasov ◽  
Ignacio Carvajal-Mariscal ◽  
...  

In vertical continuous casting machines the liquid steel from the tundish is poured into the mold through the Submerged Entry Nozzle (SEN). The shape and direction of the SEN exit jets affect the liquid steel dynamics inside the mold. This work quantifies the effect of the SEN pool on the principal characteristics of the jets emerging from it, precisely, the shape, the spread angles, and the mold impact point. Experimental and numerical simulations were carried out using a SEN simplified model, a square-shaped bore nozzle with square-shaped outlet ports whose length is minimal. These experiments showed two well-defined behaviors. When a single vortex dominates the hydrodynamics inside the simplified SEN, the exit jets spread out and are misaligned about the mold’s central plane. On the contrary, when the inner flow pattern shows two vortexes, the exit jets are compact and parallel to the mold wide walls. The measured difference on the jet’s falling angles is 5°, approximately, which implies that in an actual casting machine, the impingement point at the narrow mold wall would have a variation of 0.150 m. This hydrodynamic analysis would help design new SENs for continuous casting machines that improve steel quality.


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