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Volumn 80, Issue 4, 2009, Pages

Hidden scale invariance in molecular van der Waals liquids: A simulation study

Author keywords

[No Author keywords available]

Indexed keywords

DUMBBELL MODEL; ENERGY FLUCTUATION; EQUATION OF STATE; EQUILIBRIUM FLUCTUATION; EQUILIBRIUM POTENTIALS; MOLECULAR DYNAMICS SIMULATIONS; MOLECULAR MODELS; ORTHO-TERPHENYL; POWER-LAW; RADIAL DISTRIBUTION FUNCTIONS; SCALE INVARIANCE; SCALING EXPONENT; SCALING PROPERTIES; SIMULATION STUDIES; VAN DER WAALS;

EID: 70350230228     PISSN: 15393755     EISSN: 15502376     Source Type: Journal    
DOI: 10.1103/PhysRevE.80.041502     Document Type: Article
Times cited : (102)

References (41)
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    • The large LJ sphere, mimicking the phenyl group, is similar to the one in the Lewis-Wahnström OTP model with the parameters mp =77.106u, σp =0.4963nm and p =5.726kJ/mol. The small sphere, mimicking the methyl group, was taken from UA-OPLS with mm =15.035u, σm =0.3910nm and m =0.66944kJ/mol. Bond length: d=0.29nm. The interaction between unlike particles is determined by the Lorentz-Berthelot mixing rules.
    • The large LJ sphere, mimicking the phenyl group, is similar to the one in the Lewis-Wahnström OTP model with the parameters mp =77.106u, σp =0.4963nm and p =5.726kJ/mol. The small sphere, mimicking the methyl group, was taken from UA-OPLS with mm =15.035u, σm =0.3910nm and m =0.66944kJ/mol. Bond length: d=0.29nm. The interaction between unlike particles is determined by the Lorentz-Berthelot mixing rules.
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    • N=324molecules consisting of three LJ particles (with σ=0.483nm, ε=600K kB 4.989kJ/mol and m=76.768u) placed in the corners of a rigid isosceles triangle with two sides of length σ=0.483nm and one angle of 75°. LJ potentials were cut at rc =2.5σ using a shift function with r1 =2.3σ.
    • N=324molecules consisting of three LJ particles (with σ=0.483nm, ε=600K kB 4.989kJ/mol and m=76.768u) placed in the corners of a rigid isosceles triangle with two sides of length σ=0.483nm and one angle of 75°. LJ potentials were cut at rc =2.5σ using a shift function with r1 =2.3σ.
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    • Another issue is: what is the optimal exponent to use when correlation is not perfect? Any exponent γ Rk (k being a constant) has the required property of reducing to the pure IPL exponent in the limit of R going to one. In the present work we chose to test the exponent γ defined in Fig.
    • Another issue is: what is the optimal exponent to use when correlation is not perfect? Any exponent γ Rk (k being a constant) has the required property of reducing to the pure IPL exponent in the limit of R going to one. In the present work we chose to test the exponent γ defined in Fig..
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