× Updated! Potentials that share interactions are now listed as related models.
 
Citation: R.S. Elliott, and A. Akerson (2015), "Efficient "universal" shifted Lennard-Jones model for all KIM API supported species".

Notes: This is the Ar interaction from the "Universal" parameterization for the openKIM LennardJones612 model driver.The parameterization uses a shifted cutoff so that all interactions have a continuous energy function at the cutoff radius. This model was automatically fit using Lorentz-Berthelotmixing rules. It reproduces the dimer equilibrium separation (covalent radii) and the bond dissociation energies. It has not been fitted to other physical properties and its ability to model structures other than dimers is unknown. See the README and params files on the KIM model page for more details.

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Citation: T.X. Nguyen, S.K. Bhatia, and D. Nicholson (2005), "Prediction of High-Pressure Adsorption Equilibrium of Supercritical Gases Using Density Functional Theory", Langmuir, 21(7), 3187-3197. DOI: 10.1021/la047545h.
Abstract: In this paper, we present the results of the prediction of the high-pressure adsorption equilibrium of supercritical gases (Ar, N2, CH4, and CO2) on various activated carbons (BPL, PCB, and Norit R1 extra) at various temperatures using a density-functional-theory-based finite wall thickness (FWT) model. Pore size distribution results of the carbons are taken from our recent previous work,1,2 using this approach for characterization. To validate the model, isotherms calculated from the density functional theory (DFT) approach are comprehensively verified against those determined by grand canonical Monte Carlo (GCMC) simulation, before the theoretical adsorption isotherms of these investigated carbons calculated by the model are compared with the experimental adsorption measurements of the carbons. We illustrate the accuracy and consistency of the FWT model for the prediction of adsorption isotherms of the all investigated gases. The pore network connectivity problem occurring in the examined carbons is also discussed, and on the basis of the success of the predictions assuming a similar pore size distribution for accessible and inaccessible regions, it is suggested that this is largely related to the disordered nature of the carbon.

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Citation: G.E. Jelinek (1972), "Properties of Crystalline Argon, Krypton, and Xenon Based Upon the Born-Huang Method of Homogeneous Deformations. III. The Low-Temperature Limit", Physical Review B, 5(8), 3210-3217. DOI: 10.1103/physrevb.5.3210.
Abstract: The low-temperature limits of the thermal expansivity, specific heat, and Grüneisen parameter of solid argon, krypton, and xenon are calculated from a quasiharmonic two-body central-force model. The form of our interatomic potential and its predicted thermal and elastic properties are in good agreement with interatomic potentials for argon and krypton derived from solid-state properties plus gas viscosities, second-virial coefficients, and molecular-beam scattering data.

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Notes: Listing found at https://openkim.org.
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Notes: Listing found at https://openkim.org.
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Citation: N. Bernardes (1958), "Theory of Solid Ne, A, Kr, and Xe at 0°K", Physical Review, 112(5), 1534-1539. DOI: 10.1103/physrev.112.1534.
Abstract: A quantum-mechanical variational technique is applied to an Einstein model of a solid, and the heats of sublimation and equations of state of solid Ne, A, Kr, and Xe are calculated at 0°K. Mie-Lennard-Jones 6-12 potentials appropriate to the gas-phase data are used throughout, and the importance of quantum-mechanical effects is discussed; in general, good agreement with experiment is obtained. From the theoretical zero-point energies equivalent Debye temperatures, θ, are calculated, and from the dependence of these θ on volume, Grüneisen constants are computed in good agreement with experiment. Theoretical compressibility curves (at 0°K) are presented, and compared with the available experimental data; in the case of Ne, the only substance for which high-pressure data are available, the agreement is rather good up to 20 k atmos.

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Notes: Listing found at https://openkim.org. This KIM potential is the "low cutoff" variation.
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Notes: Listing found at https://openkim.org. This KIM potential is the "medium cutoff" variation.
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Notes: Listing found at https://openkim.org. This KIM potential is the "high cutoff" variation.
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Notes: Listing found at https://openkim.org. This KIM potential is the "smoothed" variation.
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Citation: S.J. Stuart, A.B. Tutein, and J.A. Harrison (2000), "A reactive potential for hydrocarbons with intermolecular interactions", The Journal of Chemical Physics, 112(14), 6472-6486. DOI: 10.1063/1.481208.
Abstract: A potential function is presented that can be used to model both chemical reactions and intermolecular interactions in condensed-phase hydrocarbon systems such as liquids, graphite, and polymers. This potential is derived from a well-known dissociable hydrocarbon force field, the reactive empirical bond-order potential. The extensions include an adaptive treatment of the nonbonded and dihedral-angle interactions, which still allows for covalent bonding interactions. Torsional potentials are introduced via a novel interaction potential that does not require a fixed hybridization state. The resulting model is intended as a first step towards a transferable, empirical potential capable of simulating chemical reactions in a variety of environments. The current implementation has been validated against structural and energetic properties of both gaseous and liquid hydrocarbons, and is expected to prove useful in simulations of hydrocarbon liquids, thin films, and other saturated hydrocarbon systems.

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Notes: Listing found at https://openkim.org.
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Citation: C.L. Kong, and M.R. Chakrabarty (1973), "Combining rules for intermolecular potential parameters. III. Application to the exp 6 potential", The Journal of Physical Chemistry, 77(22), 2668-2670. DOI: 10.1021/j100640a019.
Abstract: A set of combining rules for intermolecular pair potentials recently formulated and shown to be satisfactory for both the Lennard-Jones (12-6) potential and the Morse potential is applied to the exp 6 potential. Examination of the transport properties of the noble gas systems indicates that the same combining rules are also satisfacory for the exp 6 potential and, in fact, superior to the other combining rules previously suggested for the exp 6 potential model.
Citation: W. Hogervorst (1971), "Transport and equilibrium properties of simple gases and forces between like and unlike atoms", Physica, 51(1), 77-89. DOI: 10.1016/0031-8914(71)90138-8.
Abstract: A reanalysis of the transport and equilibrium properties of simple gases was performed in order to obtain more reliable parameter values for two models describing the interatomic potential, the Lennard-Jones (12-6) model and the (exp-6) model. New parameter values for the like interactions were derived from recent accurate viscosity measurements, with an exception for helium. The parameter values for the (exp-6) model differ considerably from the commonly used values given by Mason. The description of the transport properties of neon, argon, krypton and xenon is in general improved with these new parameter values. However, the description of the second virial coefficient of the considered gases with the parameter values from transport properties is rather poor. The parameter values for the unlike interactions could be calculated with several combination rules, confirming the results obtained from recent diffusion measurements in noble-gas mixtures.

Notes: The exp-6 pair potential has an exponential repulsive term and 1/6 power attractive term. Parameters due to W. Hogervorst for pure Ar and Ne are used. A mixing rule suggested by C. L. Kong and M. R. Chakrabarty is used to compute parameters for cross-interactions between Ar and Ne.

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Date Created: October 5, 2010 | Last updated: June 09, 2022