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Vortex single-celled

Barcilon Brindley, Lessen Mobbs (24) (radius ratio 0.908, r= 65) reported the disappearance of cell boundary waves at T/t = 445, but waviness continued in the interior of the vortex cells. Haji Hassan (25) showed the corresponding spectra to contain two frequencies of high power, in addition to a complex of weak frequencies. ohe two frequencies ranained up to i/t = 2500 and then disappeared. A single frequency re-emerged in the range T/T = 6000 to 60,000, the limit of the experiments. A distinctive Taylor vortex structure remained tliroughout. [Pg.400]

Fig. 26. Parameters describing diffraction from vortex lattice in superconducting UPtj as a function of field H applied along a, (a) Internal field deduced from the unit cell size. The line with slope unity is expected for singly quantized vortices, (b) Crystallographic angle a defined in the inset. For a conventional hexagonal lattice, a = 30°. (c) Scattering length, in magnetic field units, for the (1,0) Bragg reflection from the vortex lattice. (From Klerman ct al. 1992.)... Fig. 26. Parameters describing diffraction from vortex lattice in superconducting UPtj as a function of field H applied along a, (a) Internal field deduced from the unit cell size. The line with slope unity is expected for singly quantized vortices, (b) Crystallographic angle a defined in the inset. For a conventional hexagonal lattice, a = 30°. (c) Scattering length, in magnetic field units, for the (1,0) Bragg reflection from the vortex lattice. (From Klerman ct al. 1992.)...

See other pages where Vortex single-celled is mentioned: [Pg.37]    [Pg.327]    [Pg.297]    [Pg.352]    [Pg.340]    [Pg.210]    [Pg.429]    [Pg.256]    [Pg.282]    [Pg.37]    [Pg.37]    [Pg.143]    [Pg.204]    [Pg.33]    [Pg.251]    [Pg.104]    [Pg.419]    [Pg.211]    [Pg.342]    [Pg.89]   
See also in sourсe #XX -- [ Pg.297 ]




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