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Finite-size excess-entropy scaling for simple liquids
Mauricio Sevilla1, Atreyee Banerjee1, Robinson Cortes-Huerto1
1Max Planck Institute for Polymer Research, Ackermannweg 10, 55128 Mainz, Germany.
The Journal of Chemical Physics
|May 23, 2023
Summary
Computer simulations reveal how system size affects diffusion. Reduced self-diffusion coefficients and excess entropy scale linearly with inverse system size, suggesting a constant viscosity-to-entropy ratio.
Area of Science:
- Computational physics
- Statistical mechanics
Background:
- Computer simulations in physics often exhibit size effects.
- Explicit and implicit size effects arise from fixed particle numbers and periodic boundary conditions, respectively.
Purpose of the Study:
- Investigate size effects on the relationship between reduced self-diffusion coefficient (D*(L)) and two-body excess entropy (s2(L)).
- Analyze the scaling behavior of D*(L) and s2(L) with system size (L).
Main Methods:
- Introduced and validated a finite-size two-body excess entropy integral equation.
- Performed computer simulations for prototypical simple-liquid systems.
- Analyzed the linear scaling of s2(L) with 1/L and D*(L) with system size.
Main Results:
- Demonstrated that s2(L) scales linearly with 1/L.
- Showed that D*(L) exhibits similar linear scaling behavior.
- Found that parameters A(L) and α(L) are linearly proportional to 1/L.
- Extrapolated to the thermodynamic limit, yielding coefficients A∞ = 0.048 ± 0.001 and α∞ = 1.000 ± 0.013.
Conclusions:
- The study confirms universal values for A∞ and α∞, consistent with prior literature.
- A power law relation between scaling coefficients suggests a constant viscosity-to-entropy ratio in simple liquids.
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