On the arrangement of monovariant lines in two-dimensional potential phase diagrams

1985 ◽  
Vol 16 (1) ◽  
pp. 137-139 ◽  
Author(s):  
Mats Hillert
2000 ◽  
Vol 3 (1) ◽  
pp. 63-70 ◽  
Author(s):  
C. Alonso ◽  
F. Artzner ◽  
J. Lajzerowicz ◽  
G. Grubel ◽  
N. Boudet ◽  
...  

1985 ◽  
Vol 46 (C3) ◽  
pp. C3-47-C3-60 ◽  
Author(s):  
R. M. Hornreich ◽  
M. Kugler ◽  
S. Shtrikman

2008 ◽  
Vol 73 (3) ◽  
pp. 372-387 ◽  
Author(s):  
Petr Voňka ◽  
Jindřich Leitner ◽  
David Sedmidubský

An analysis of topology of two-dimensional isothermal potential phase diagrams of partially open immiscible condensed systems is presented. The systems share two independent components with surroundings. Chemical potentials (or derived properties such as activities or relative partial pressures) of these two independent components are used as coordinates of such diagrams. Several theorems on topology having practical consequences are proved.


1985 ◽  
Vol 18 (1) ◽  
pp. 73-82 ◽  
Author(s):  
R Badke ◽  
P Reinicke ◽  
V Rittenberg

2011 ◽  
Vol 22 (07) ◽  
pp. 661-668 ◽  
Author(s):  
NAJEM MOUSSA ◽  
ILIASS TARRAS ◽  
M'HAMMED MAZROUI ◽  
YAHYA BOUGHALEB

In nature many animal groups, such as fish schools or bird flocks, clearly display structural order and appear to move as a single coherent entity. In order to understand the complex behavior of these systems, many models have been proposed and tested so far. This paper deals with an extension of the Vicsek model, by including a second zone of repulsion, where each agent attempts to maintain a minimum distance from the others. The consideration of this zone in our study seems to play an important role during the travel of agents in the two-dimensional (2D) flocking models. Our numerical investigations show that depending on the basic ingredients such as repulsion radius (R1), effect of density of agents (ρ) and noise (η), our nonequilibrium system can undergo a kinetic phase transition from no transport to finite net transport. For different values of ρ, kinetic phase diagrams in the plane (η ,R1) are found. Implications of these findings are discussed.


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