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Comments on the numerical simulations of electrolytes in periodic boundary conditions
Relying on the article of de Leeuw, Perram, and Smith [Proc. R. Soc. London, Ser. A 373, 27 (1980)] we justify the expression of the Hamiltonian actually used in the numerical simulations of electrolyte solutions in a periodic geometry. It involves the itinerant dipole moment Mi of the charges rathe...
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Published in: | The Journal of chemical physics 1994-10, Vol.101 (7), p.6080-6090 |
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Main Author: | |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Relying on the article of de Leeuw, Perram, and Smith [Proc. R. Soc. London, Ser. A 373, 27 (1980)] we justify the expression of the Hamiltonian actually used in the numerical simulations of electrolyte solutions in a periodic geometry. It involves the itinerant dipole moment Mi of the charges rather than the electric moment MB of the simulation box. The vector Mi is defined as the electric moment of the particles which were in the simulation box at t=0 and may have diffused away in the neighboring cells in the course of the simulation. Some comments on Stillinger–Lovett conditions are included. |
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ISSN: | 0021-9606 1089-7690 |
DOI: | 10.1063/1.468422 |