Statistical geometry of some dense random packing of hard spheres model structures

1986 ◽  
Vol 81 (1-2) ◽  
pp. 13-28 ◽  
Author(s):  
L. Takács
Nature ◽  
1969 ◽  
Vol 224 (5219) ◽  
pp. 550-553 ◽  
Author(s):  
R. H. BERESFORD

1982 ◽  
Vol 37 (6) ◽  
pp. 611-612 ◽  
Author(s):  
T. Fujiwara ◽  
H. S. Chen ◽  
Y. Waseda

Abstract Three partial radial distribution functions [RDF’s] are calculated by means of relaxed dense-random packing models for a Fe80B20 glass. The model structures reproduce fairly well recently reported experimental partial RDF's derived from x-ray diffraction and neutron diffraction using isotopic substitutional methods. Most significantly, both the model calculated by means of relaxed dense-random packing models GBB (r), the appearance of a subpeak on the short distance side of the first peak.


1991 ◽  
Vol 176 (2) ◽  
pp. 206-219 ◽  
Author(s):  
A. Pavlovitch ◽  
R. Jullien ◽  
P. Meakin

1981 ◽  
Vol 8 ◽  
Author(s):  
M. E. Eberhart ◽  
K. H. Johnnson ◽  
R. C. O'Handley

ABSTRACTSCF-Xα-SW calculations have been performed on the glass forming crystal of Ni2B. The resulting molecular orbital topology near the fermi level is similar to that previously obtained by SCF-Xα-SW calculation on the glass forming crystals of Pd-Si and Cu-Zr. These similarties, it is conjectured, indicate melting is an electronically driven phase transition and that liquid and glass structures are more the result of electronic than kinetic factors. It is shown that the molecular orbital model of melting in transition metals will generate structures similar to those resulting from the dense random packing of hard spheres method, and the molecualr orbital mechanism admits, in a qualitative way, the explanation of a broad range of liquid and glass properties.


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