Abstract
Monte Carlo and molecular dynamics simulations are, in principle, powerful tools for carrying out the basic task of statistical thermodynamics, namely the prediction of macroscopic properties of matter from suitable models of effective interactions between atoms and molecules. The state of the art of this approach is reviewed, with an emphasis on solutions of rather short polymer chains (such as alkanes) in various solvents. Several methods of constructing coarse-grained models of the simple bead–spring type will be mentioned, using input either from atomistic models (considering polybutadiene as an example) or from experiment. Also, the need to have corresponding coarse-grained models of the solvent molecules is emphasized, and examples for various dipolar and quadrupolar fluids and their mixtures with short alkanes are given. Finally, we mention even more simplified models, such as the bond fluctuation model on the simple cubic lattice, treating applications like micelle formation in block copolymer solutions or isotropic–nematic phase transitions in solutions of stiff polymers as case studies. Comparisons with pertinent predictions from approximate analytical theories will be briefly mentioned, as well as applications, to understand experimental results.
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- AO:
-
Asakura–Oosawa model
- CMC:
-
Critical micelle concentration
- DPD:
-
Dissipative particle dynamics
- EPM:
-
Elementary physical model
- EPM2:
-
Second elementary physical model
- FENE:
-
Finitely extensible nonlinear elastic
- GEMC:
-
Gibbs ensemble Monte Carlo
- LJ:
-
Lennard–Jones
- MC:
-
Monte Carlo
- MD:
-
Molecular dynamics
- NIST:
-
National Institute of Standards and Technology
- \(\mathcal{N}pT\) :
-
Constant particle number, constant pressure, and constant temperature ensemble
- \(\mathcal{N}VE\) :
-
Constant particle number, constant volume, and constant energy ensemble (= microcanonical ensemble)
- \(\mathcal{N}VT\) :
-
Constant particle number, constant volume, and constant temperature ensemble (= canonical ensemble)
- PC-SAFT:
-
Perturbed-chain statistical associating fluid theory
- rRESPA:
-
Reversible reference systems propagator algorithm
- SAFT:
-
Statistical associating fluid theory
- SAW:
-
Self-avoiding walk
- SCFT:
-
Self-consistent field theory
- SM:
-
Stockmayer model
- SW:
-
Square well
- TI\(\mu VT\) :
-
Thermodynamic integration in the constant chemical potential, constant volume, and constant temperature ensemble
- TPT:
-
Thermodynamic perturbation theory
- TPT1-MSA:
-
First-order thermodynamic perturbation theory combined with the mean spherical approximation
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Acknowledgement
Part of the work reviewed here has been carried out in a fruitful and productive collaboration with A. Cavallo, V. Ivanov, L. G. MacDowell, M. Müller, M. Oettel, and T. Strauch; it is a pleasure to thank them. Stimulating discussions with H. Weiss and F. Heilmann are acknowledged as well. Financial support has been provided by the BASF SE and by the Deutsche Forschungsgemeinschaft (DFG) in the framework of projects DFG 436 RUS 113/791, PA473/7-1 and PA473/8-1, and Sonderforschungsbereich 625. Computer time grants were provided by John von Neumann Institute for Computing (NIC) and the Network of Excellence SOFTCOMP.
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Binder, K., Mognetti, B., Paul, W., Virnau, P., Yelash, L. (2010). Computer Simulations and Coarse-Grained Molecular Models Predicting the Equation of State of Polymer Solutions. In: Wolf, B., Enders, S. (eds) Polymer Thermodynamics. Advances in Polymer Science, vol 238. Springer, Berlin, Heidelberg. https://doi.org/10.1007/12_2010_82
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