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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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40 Koichiro Nakanishi<br />

Figure 2.2.1. A scheme for the design <strong>of</strong> molecular ensembles.<br />

sion <strong>of</strong> additivity rule, which has now an empirical character. It is however useful for practical<br />

purposes.<br />

2.2.5 MODEL SYSTEM AND PARADIGM FOR DESIGN<br />

The method described above is so to speak an orthodox approach and the ability <strong>of</strong> present-day’s<br />

supercomputer is still a high wall in the application <strong>of</strong> molecular simulation. Then<br />

the role <strong>of</strong> the second method given in the last section is highly expected.<br />

It is the method with empirical potential model. As the model, the approximation that<br />

any molecule can behave as if obeying Lennard-Jones potential seems to be satisfactory.<br />

This (one-center) LJ model is valid only for rare gases and simple spherical molecules. But<br />

this model may also be valid for other simple molecules as a zeroth approximation. We may<br />

also use two-center LJ model where interatomic interactions are concentrated to the major<br />

two atoms in the molecule. We expect that these one-center and two-center LJ models will<br />

play a role <strong>of</strong> Occam’s razor.<br />

We propose a paradigm for physical properties prediction as shown in Figure 2.2.1.<br />

This corresponds to the stage (2) and may be used to prepare the process <strong>of</strong> stage (3),<br />

namely, the molecular ensemble design for solvents.<br />

Main procedures in this paradigm are as follows; we first adopt target molecule or<br />

mixture and determine their LJ parameters. At present stage, LJ parameters are available<br />

only for limited cases. Thus we must have method to predict effective LJ parameters.

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