This work examines a correction to the Helmholtz free energy arising from anisotropy of pair and three-body non-additive interactions. The corrections are derived for axially symmetric molecules through the third order of a perturbation treatment. The effects of higher-order terms are then approximated by means of a simple Padé extrapolation procedure. A Lennard-Jones (12-6) potential is assumed to describe the spherically symmetric component of the two-body potential for overlap and dispersion interactions. The numerical results are given for the force parameters which are used to describe the gaseous properties of CO<SUB>2</SUB>, HCl and NH<SUB>3</SUB> molecules
We propose a new thermodynamic approach for nonspherical molecules by applying a perturbation theory...
The initial part of this work is concerned with the construction and validity of model potential ene...
199-203A new non-equilibrium statistical thermodynamics perturbation theory was developed which cou...
The thermodynamic perturbation theory in which all angle-dependent interactions are considered as a ...
The application of thermodynamic perturbation theory in which all tensor interactions are taken as p...
Computationally convenient theoretical methods for calculating the structural and thermodynamic prop...
Perturbation theory is used to consider the effect of the three-body potential on the radial distrib...
Nonadditive effects are calculated for (HF)3 and (HCl)3 complexes and analyzed via the combination o...
A new one-parameter correction scheme to second-order Møller–Plesset many-body perturbation theory (...
A modified, computationally efficient method to provide permutationally invariant polynomial bases f...
Advances in molecular simulation algorithms coupled with rapid growth in the calculation speed of mo...
The equilibrium properties of anisotropic molecular fluids can be in principle calculated in a stati...
$^{1}$ G.C. Maitland, M. Rigby, E.B. Smith, and W.A. Wakeham, Intermolecular Forces (Clarendon, Oxfo...
The Percus-Yevick (PY) integral equation has been solved for two model fluids: (i) a fluid of hard e...
This research is involved with the construction of potential energy models for the interaction of cl...
We propose a new thermodynamic approach for nonspherical molecules by applying a perturbation theory...
The initial part of this work is concerned with the construction and validity of model potential ene...
199-203A new non-equilibrium statistical thermodynamics perturbation theory was developed which cou...
The thermodynamic perturbation theory in which all angle-dependent interactions are considered as a ...
The application of thermodynamic perturbation theory in which all tensor interactions are taken as p...
Computationally convenient theoretical methods for calculating the structural and thermodynamic prop...
Perturbation theory is used to consider the effect of the three-body potential on the radial distrib...
Nonadditive effects are calculated for (HF)3 and (HCl)3 complexes and analyzed via the combination o...
A new one-parameter correction scheme to second-order Møller–Plesset many-body perturbation theory (...
A modified, computationally efficient method to provide permutationally invariant polynomial bases f...
Advances in molecular simulation algorithms coupled with rapid growth in the calculation speed of mo...
The equilibrium properties of anisotropic molecular fluids can be in principle calculated in a stati...
$^{1}$ G.C. Maitland, M. Rigby, E.B. Smith, and W.A. Wakeham, Intermolecular Forces (Clarendon, Oxfo...
The Percus-Yevick (PY) integral equation has been solved for two model fluids: (i) a fluid of hard e...
This research is involved with the construction of potential energy models for the interaction of cl...
We propose a new thermodynamic approach for nonspherical molecules by applying a perturbation theory...
The initial part of this work is concerned with the construction and validity of model potential ene...
199-203A new non-equilibrium statistical thermodynamics perturbation theory was developed which cou...