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Lecture 7: Distribution functions in classical monatomic liquids

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1 Lecture 7: Distribution functions in classical monatomic liquids
Statistical Thermodynamics Lecture 7: Distribution functions in classical monatomic liquids Dr. Ronald M. Levy

2 Liquids behaves different from gas
For imperfect gases, virial equation of state could be written as a sum of configurational integrals, involving 1 body, 2 body, 3 body, … For liquids, this expansion gives poor results. For liquids, it is not a good approximation to treat the system as a sequence of 1 body, 2 body, 3 body … etc. Hard sphere equation of state liquid solid MD simulation - liquid MD simulation - solid V0/V 1

3 1 2 3 N particle potential Conformational partition function
N particle potential 1 Conformational partition function Integrated over n+1 to N 2 3 2

4 n particle correlation function
n particle correlation function 4 3

5 5 This equation defines the Conditional probability 4

6 N 1 6 5

7 6

8 Mean kinetic energy Mean potential energy 7

9 7 Expression for average internal energy in terms of pair correlation function 8

10 Double count Averge potential energy between molecule1 and molecules locates between r and r+dr N identical terms 8 9

11 9 10 The factor V comes from the integration of dr
9 The factor V comes from the integration of dr coupling parameter integration 10 10

12 11 There are N-1 identical terms leading to N-1 identical integrals
There are N-1 identical terms leading to N-1 identical integrals 11 Depends on coupling parameter 11

13 12 13 12

14 Potential of mean force(potential which gives the mean force) 14 13

15 15 Direct+indirect indirect
15 Measure of the total influence of mol1 and mol2 Indirect part is the direct influence of particle 1 on 3. which in turn exerts its influence on 2 directly or indirectly The direct correlation function is defined by this equation Direct+indirect indirect Can solve 2 equation interatively 14

16 Set of solute coordinates
Set of solute coordinates Set of solvent coordinates Potential energy of the system Defines W (PMF) 15

17 16

18 Solute charge distribution
Solvent induced influence Intramolecular solute potential Solute charge distribution Poisson equation 17


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