view article
Figure 1
(a) Nonideal parts of the chemical potentials [\beta \mu _{1}^{\rm ni}] and [\beta \mu _{2}^{\rm ni}] shown as functions of the number of particles N for model A. The symbols represent the values obtained by MC simulations. Data were collected at 21 values of the mole fraction X1. Here results are presented for only a few representative values of X1: 0.00 (circles), 0.25 (crosses), 0.50 (squares), 0.75 (triangles, upward) and 1.00 (triangles, downward). The results shown here were all collected at the same volume of the MC cell, equal to 106 nm3. Thus the number density ρ is equal to 10−6N. The curves are the best fitting polynomials, equation (6)[link]. The maximum values of the volume fraction η range from 0.23 (circles) to 0.37 (triangles, downward). (b) Nonideal parts of the chemical potentials [\beta \mu _{1}^{\rm ni}] and [\beta \mu _{2}^{\rm ni}] shown as functions of N for model B. Further details are as for (a). The maximum value of the volume fraction η is 0.35.

Journal logoJOURNAL OF
APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
Volume 36| Part 5| October 2003| Pages 1128-1134
https://doi.org/10.1107/S0021889803012615
Follow J. Appl. Cryst.
Sign up for e-alerts
E-alerts
Follow J. Appl. Cryst. on Twitter
Twitter
Follow us on facebook
Facebook
Sign up for RSS feeds
RSS