High critical flux density gradients near the surface of superconducting niobium

1979 ◽  
Vol 36 (1-2) ◽  
pp. 33-46 ◽  
Author(s):  
A. S. Brito ◽  
G. Zerweck ◽  
O. F. de Lima



1980 ◽  
Vol 60 (2) ◽  
pp. 417-426 ◽  
Author(s):  
R. Potratz ◽  
W. Klein ◽  
H. U. Habermeier ◽  
H. Kronmüller


2019 ◽  
Vol 631 ◽  
pp. A65 ◽  
Author(s):  
R. Cesaroni

We consider a dusty clump in two cases of spherical and cylindrical symmetry to investigate the effect of temperature and density gradients on the observed flux density. Conversely, we evaluate how the presence of these gradients affects the calculation of the clump mass from the observed flux. We provide approximate expressions relating flux density and mass in the optically thick and thin limits and in the Rayleigh-Jeans regime, and we discuss the reliability of these expressions by comparing them to the outcome of a numerical code. Finally, we present the application of our calculations to three examples taken from the literature, which shows how the correction introduced after taking into account temperature and density gradients may affect our conclusions on the stability of the clumps.



1991 ◽  
Vol 185-189 ◽  
pp. 2335-2336 ◽  
Author(s):  
Alexander Forkl ◽  
Hanns-Ulrich Habermeier ◽  
Bernd Leibold ◽  
Helmut Kronmüller


1990 ◽  
Vol 166 (1-2) ◽  
pp. 36-48 ◽  
Author(s):  
M.R. Koblischka ◽  
N. Moser ◽  
B. Gegenheimer ◽  
H. Kronmüller




Cryogenics ◽  
1976 ◽  
Vol 16 (1) ◽  
pp. 39-41 ◽  
Author(s):  
H.W. Weber ◽  
G.P. Westphal ◽  
I. Adaktylos


1977 ◽  
Vol 26 (3-4) ◽  
pp. 533-544 ◽  
Author(s):  
I. Adaktylos ◽  
E. Schachinger ◽  
H. W. Weber


1978 ◽  
Vol 39 (C6) ◽  
pp. C6-635-C6-637
Author(s):  
H. U. Habermeier ◽  
W. Klein ◽  
H. Kronmüller


Author(s):  
M. Strojnik

Magnetic lenses operating in partial saturation offer two advantages in HVEM: they exhibit small cs and cc and their power depends little on the excitation IN. Curve H, Fig. 1, shows that the maximal axial flux density Bz max of one of the lenses investigated changes between points (3) and (4) by 5% as the excitation varies by 40%. Consequently, the designer can relax the requirements concerning the stability of the lens current supplies. Saturated lenses, however, can only be used if (i) unwanted fields along the optical axis can be controlled, (ii) 'wobbling' of the optical axis due to inhomogeneous saturation around the pole piece faces is prevented, (iii) ample ampere-turns can be squeezed into the space available, and (iv) the lens operating point covers a sufficient range of accelerating voltages.



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