Structures of single vortex and vortex lattice in ad-wave superconductor

1996 ◽  
Vol 53 (6) ◽  
pp. R2991-R2994 ◽  
Author(s):  
Ji-Hai Xu ◽  
Yong Ren ◽  
Chin-Sen Ting
Keyword(s):  
2014 ◽  
Vol 115 (6) ◽  
pp. 063906 ◽  
Author(s):  
D. Mitin ◽  
D. Nissen ◽  
P. Schädlich ◽  
S. S. P. K. Arekapudi ◽  
M. Albrecht

2010 ◽  
Vol 81 (1) ◽  
Author(s):  
D. S. Inosov ◽  
T. Shapoval ◽  
V. Neu ◽  
U. Wolff ◽  
J. S. White ◽  
...  

1993 ◽  
Vol 07 (15) ◽  
pp. 999-1011 ◽  
Author(s):  
G. NARSINGA RAO ◽  
D. SURESH BABU ◽  
P. MOLINIE ◽  
M. GANNE

We report characterization and detailed magnetization study in fields up to 2 T in the temperature range between 5 and 80 K of Bi 1.6 Pb 0.3 W 0.1 Sr 2 Ca 2 Cu 3 O y (nominal composition pellets). XRD, field-cooled magnetization measurements, and electrical resistance studies showed that the sample consists of a single phase high-Tc (Bi-2223) superconductor in addition to CaWO y-type impurity. An empirical magnetic phase diagram of the superconducting system has been derived. We determined a H*(T) line where Jc becomes zero. In the region with nonzero critical current density, vortex lattice exhibits mainly two types of pinning behaviours, single vortex and collective pinning behaviour, in different field and temperature range. In addition, the temperature dependence of Jc showed an evidence of two types of pinning centres. In low temperatures (<40 K), the pinning centers with low values of activation energy are active whereas in high temperatures (≥40 K), the pinning centers with larger activation energy are active. These results are compared with those of Job & Rosenberg1 on Bi-2223 ceramic samples.


1996 ◽  
Vol 10 (22) ◽  
pp. 2699-2721 ◽  
Author(s):  
JI-HAI XU ◽  
YONG REN ◽  
C. S. TING

YBa 2 Cu 3 O 7 (YBCO) exhibits a large anisotropy between the a (or y) and b (or x) axes in the CuO2 planes. This anisotropy can be modeled by introducing an anisotropic mass parameter λ = mx /my. Assuming a d-wave pairing interaction together with a repulsive on-site Coulomb interaction, we developed a Ginzburg–Landau theory for a d-wave superconductor with mass anisotropy in the presence of a magnetic field. We show that the order parameter always has s + d symmetry. The vortex structures for λ = 1 and λ > 1 have been numerically studied. For high T c cuprates with tetragonal structure (λ = 1), the vortex shows a four-fold symmetry and the vortex lattice may have oblique or triangular structure depending on the strength of the applied magnetic field, temperature, and the other parameters. For YBCO we choose λ = 2, the single vortex has an elliptic shape, and the vortex lattice always shows an oblique structure. All these results are in good agreement with experimental measurements.


1992 ◽  
Vol 275 ◽  
Author(s):  
Shinya Tokuono ◽  
Shoji Tanaka ◽  
Hidetoshi Fukuyama

ABSTRACTInteraction between vortices and inhomogeneity in superconductors is studied. As a typical example, we investigated the case of a single vortex and some vortices near an inclusion of the cylindrical shape and derived the interaction potential for the vortices as a function of the distance by use of the solution of London equation.


AIAA Journal ◽  
1997 ◽  
Vol 35 ◽  
pp. 1230-1233
Author(s):  
Paulo A. O. Soviero ◽  
Hugo B. Resende

AIAA Journal ◽  
2002 ◽  
Vol 40 ◽  
pp. 1187-1196
Author(s):  
J.-N. Juang ◽  
D. Kholodar ◽  
E. H. Dowell

2019 ◽  
Vol 2019 ◽  
pp. 1-15
Author(s):  
Sen Mao ◽  
Changchuan Xie ◽  
Lan Yang ◽  
Chao Yang

A morphing trailing-edge (TE) wing is an important morphing mode in aircraft design. In order to explore the static aeroelastic characteristics of a morphing TE wing, an efficient and feasible method for static aeroelastic analysis has been developed in this paper. A geometrically exact vortex lattice method (VLM) is applied to calculate the aerodynamic forces. Firstly, a typical model of a morphing TE wing is chosen and built which has an active morphing trailing edge driven by a piezoelectric patch. Then, the paper carries out the static aeroelastic analysis of the morphing TE wing and corresponding simulations were carried out. Finally, the analysis results are compared with those of a traditional wing with a rigid trailing edge using the traditional linearized VLM. The results indicate that the geometrically exact VLM can better describe the aerodynamic nonlinearity of a morphing TE wing in consideration of geometrical deformation in aeroelastic analysis. Moreover, out of consideration of the angle of attack, the deflection angle of the trailing edge, among others, the wing system does not show divergence but bifurcation. Consequently, the aeroelastic analysis method proposed in this paper is more applicable to the analysis and design of a morphing TE wing.


2019 ◽  
Vol 30 (7) ◽  
pp. 6688-6692
Author(s):  
V. I. Beletskiy ◽  
G. Ya. Khadzhai ◽  
R. V. Vovk ◽  
N. R. Vovk ◽  
A. V. Samoylov ◽  
...  

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.


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