Abstract

The first objective of this paper is to investigate the scaling behavior of liquid-vapor phase transition in FCC and BCCmetals starting from the zero-temperature four-parameter formula for cohesive energy. The effective potentials between the atoms in the solid are determined while using lattice inversion techniques as a function of scaling variables in the four-parameter formula. These potentials are split into repulsive and attractive parts, as per the Weeks–Chandler–Anderson prescription, and used in the coupling-parameter expansion for solving the Ornstein–Zernike equation that was supplemented with an accurate closure. Thermodynamic quantities obtained via the correlation functions are used in order to obtain critical point parameters and liquid-vapor phase diagrams. Their dependence on the scaling variables in the cohesive energy formula are also determined. An equally important second objective of the paper is to revisit coupling parameter expansion for solving the Ornstein–Zernike equation. The Newton–Armijo non-linear solver and Krylov-space based linear solvers are employed in this regard. These methods generate a robust algorithm that can be used to span the entire fluid region, except very low temperatures. The accuracy of the method is established by comparing the phase diagrams with those that were obtained via computer simulation. The avoidance of the ’no-solution-region’ of the Ornstein-Zernike equation in coupling-parameter expansion is also discussed. Details of the method and complete algorithm provided here would make this technique more accessible to researchers investigating the thermodynamic properties of one component fluids.

Highlights

  • The scaling and universal features in phase transition theory were first brought out with the van der Waals equation of state [1]

  • The mean field approach implied in the van der Waals equation neglects long range fluctuations that are close to the critical point and so provide only the classical critical behavior as opposed to the renormalization group theory of critical phenomena [2]

  • The four-parameter formula for cohesive energy expressed in units E0 and L0 consists of just two dimensionless variables (η and δ)

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Summary

Introduction

The scaling and universal features in phase transition theory were first brought out with the van der Waals equation of state [1]. It is natural to explore whether the universal energyvolume curve can be extended to the expanded volume states to describe the liquid-vapor phase transition in metallic fluids [5] This investigation becomes easy when used with the corrected rigid spheres (CRIS) model, which is a thermodynamic perturbation theory that. Effective pair interaction potentials are derived from the SCE formula by employing lattice inversion techniques, and split into repulsive and attractive components while using the Weeks–Chandler–Anderson (WCA) prescription [10] These components are used in an accurate thermodynamic perturbation theory, called couplingparameter expansion (CPE) [11], for solving the Ornstein-Zernike equation (OZE) and an appropriate closure relation. The critical point parameters and phase diagrams of metallic fluids are obtained in terms of the scaling variables in the SCE formula. The Appendix A provides details of the complete algorithm for easy implementation of CPE

Scaled Cohesive Energy Formula
Lattice Inversion for Potential
15. There is no shell of radius
Inter-Particle Potentials for FCC and BCC Metals
F C C r m in r m in u u m in η m in 0 η
Coupling-Parameter Expansion
Newton-Armijo Solver for Reference System
Derivatives of Correlation Functions
Derivatives of Bridge Function
Thermodynamic Functions
Liquid-Vapor Phase Transition in Metals
Summary
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