| Original language | English (US) |
|---|---|
| Pages (from-to) | 173-214 |
| Number of pages | 42 |
| Journal | Advances in colloid and interface science |
| Volume | 10 |
| Issue number | 1 |
| DOIs | |
| State | Published - Jan 1979 |
| Externally published | Yes |
All Science Journal Classification (ASJC) codes
- Surfaces and Interfaces
- Physical and Theoretical Chemistry
- Colloid and Surface Chemistry
Access to Document
Other files and links
Cite this
- APA
- Author
- BIBTEX
- Harvard
- Standard
- RIS
- Vancouver
}
Computer experiments on phase separation in binary alloys. / Binder, K.; Kalos, M. H.; Lebowitz, J. L. et al.
In: Advances in colloid and interface science, Vol. 10, No. 1, 01.1979, p. 173-214.Research output: Contribution to journal › Article › peer-review
TY - JOUR
T1 - Computer experiments on phase separation in binary alloys
AU - Binder, K.
AU - Kalos, M. H.
AU - Lebowitz, J. L.
AU - Marro, J.
N1 - Funding Information: CONTENTS I. Introduction ____._.__________._______________________________.___.__1_73_ II. Experimental situation .._.__._._.-...._____-..-.____----..___.-------1-7 s - III. Discussion of theoretical concepts ______________.______-_____.-______1-7 9 A. Macroscopic theory .._..*___....___*_*_*..-_____*_--______.__-----1_7 9 B. Theories including fluctuations _____.__________._.__.........____1_5 2 C. Theories for the asymptotic time-dependence of the coarsening .. . . . 185 IV. Simple microscopic lattice models of binary alloys ___..______.______..1 88 A. Equilibrium properties .____________.________________...__.____~~_1_8 8 B. Time-dependent properties ____...____._....____......__._.........1.9 1 V. Computer simulation of time evolution _.___.......___......___._.......1 93 A. Description of the model _...____.___..__.___-...______......__.__1_9 3 B. Results .______.._______.________._____..__..___._...___.........1.9.6 VI. Discussion and conclusions ______..________...____.____________.______2_1 -O INTRODUCTION A binary alloy, such as ZnAt, is spatially homogeneous when it is in thermal equilibrium at sufficiently high temperatures; that is, it consists of one thermodynamic phase. If the system is suddenly quenched to a lower temperature (see Fig. l), it remains spatially homogeneous. Thermal equilibrium, however; requires the coexistence of two phases, one A-rich and one B-rich, whenever the fraction of "B-atoms" E is in the range cAccccB in Fig. 1. The nature of the time evolution 'Work supported by AFOSR Grant No.73-2430B and E.R.D.A. Contract No.AT(ll-I)-3077. 'tpermanent address: Departamento de Fisica Teorica. Universidad de Barcelona, and Instituto de Fisica Te&ica de1 C.S.I.C., Barcelona-14, Spain. Partially supported by the Program for Cultural Interchange between Spain and the U.S.A. and the Fulbright-Hays Program, Madrid, Spain-
PY - 1979/1
Y1 - 1979/1
UR - http://www.scopus.com/inward/record.url?scp=0018326132&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=0018326132&partnerID=8YFLogxK
U2 - 10.1016/0001-8686(79)87006-2
DO - 10.1016/0001-8686(79)87006-2
M3 - Article
AN - SCOPUS:0018326132
VL - 10
SP - 173
EP - 214
JO - Advances in Colloid and Interface Science
JF - Advances in Colloid and Interface Science
SN - 0001-8686
IS - 1
ER -