FLUX DENSITY GRADIENTS IN PLASTICALLY DEFORMED NIOBIUM SINGLE CRYSTALS

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

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


1994 ◽  
Vol 18 (2) ◽  
pp. 695-698
Author(s):  
T. Kubo ◽  
Y. Yokoyama ◽  
K. Oka ◽  
D.H. Ha ◽  
S. Arai ◽  
...  


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


Author(s):  
Lucien F. Trueb

A new type of synthetic industrial diamond formed by an explosive shock process has been recently developed by the Du Pont Company. This material consists of a mixture of two basically different forms, as shown in Figure 1: relatively flat and compact aggregates of acicular crystallites, and single crystals in the form of irregular polyhedra with straight edges.Figure 2 is a high magnification micrograph typical for the fibrous aggregates; it shows that they are composed of bundles of crystallites 0.05-0.3 μ long and 0.02 μ. wide. The selected area diffraction diagram (insert in Figure 2) consists of a weak polycrystalline ring pattern and a strong texture pattern with arc reflections. The latter results from crystals having preferred orientation, which shows that in a given particle most fibrils have a similar orientation.



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