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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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2.1 Solvent effects on chemical systems 19<br />

If we are capable <strong>of</strong> integrating the equations <strong>of</strong> movement <strong>of</strong> all the particles which<br />

constitute a system, we can find their paths and velocities and we can evaluate the properties<br />

<strong>of</strong> the system in determined time intervals. Thus, we can find how the system being studied<br />

evolved as time moves forward. In the first simulations by Molecular Dynamics <strong>of</strong> a condensed<br />

phase, 34 use was made <strong>of</strong> potentials as simple as the hard sphere potential, under<br />

which the constituent particles move in a straight line until colliding elastically. The collisions<br />

happen when the separation between the centers <strong>of</strong> the spheres is equal to the diameter<br />

<strong>of</strong> the sphere. After each collision, the new velocities are obtained by making use <strong>of</strong> the<br />

principle <strong>of</strong> conservation <strong>of</strong> the linear moments. But a chemical system requires more elaborate<br />

potentials under which the force, which at every instant acts between two atoms or<br />

molecules, changes in relation to the variation <strong>of</strong> the distance between them. This obliges us<br />

to integrate the equations <strong>of</strong> movement <strong>of</strong> the system in very small time intervals, in which it<br />

is assumed that the force which acts on each atom or molecule is constant, generally lying<br />

between 1 and 10 femtoseconds. For each <strong>of</strong> these intervals, the positions and velocities <strong>of</strong><br />

each <strong>of</strong> the atoms is calculated, after which they are placed in their new positions and, once<br />

again, the forces are evaluated to obtain the parameters <strong>of</strong> a new interval, and so on, successively.<br />

This evolution in time, which usually requires the evaluation <strong>of</strong> hundreds <strong>of</strong> thousands<br />

<strong>of</strong> intervals <strong>of</strong> approximately 1 femtosecond each, allows us to know the properties <strong>of</strong><br />

the system submitted to study during the elapse <strong>of</strong> time. In fact, the task commences by fixing<br />

the atoms which make up the system being studied in starting positions, and later move<br />

them continuously whilst the molecules being analysed rotate, the bond angles bend, the<br />

bonds vibrate, etc., and during which the dispositions <strong>of</strong> the atoms which make up the system<br />

are tabulated at regular intervals <strong>of</strong> time, and the energies and other properties which<br />

depend on each <strong>of</strong> the conformations, through which the molecular system makes its way<br />

with the passage <strong>of</strong> time, are evaluated. Molecular Dynamics is Chemistry scrutinized each<br />

femtosecond.<br />

Monte Carlo methods<br />

The first simulation by computer <strong>of</strong> a molecular system was carried out using this method.<br />

It consists <strong>of</strong> generating configurations <strong>of</strong> a system introducing random changes in the position<br />

<strong>of</strong> its constituents.<br />

In order to obtain a good convergence in the sequence <strong>of</strong> configurations, Metropolis et<br />

al. 35 suggested an interesting approach. This approach avoids the generation <strong>of</strong> a very long<br />

random configurations as follows: instead <strong>of</strong> choosing random configurations and then<br />

weighing them according to the Boltzmann factor, one generates configurations with a<br />

probability equal to the Boltzmann factor and afterwards weigh them evenly. For this purpose<br />

once a new configuration is generated the difference in the potential energy with respect<br />

to the previous one is computed (ΔU) and a random number 0 ≤r ≤1 is selected. If the<br />

Boltzmann factor exp(-ΔU/kT)>r then the new configuration is accepted, if exp(-ΔU/kT)

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