KNOWPIA
WELCOME TO KNOWPIA

- Summary
- Physical background and mathematical details
- Application of the Lennard-Jones potential in molecular modeling
- Alternative notations of the Lennard-Jones potential
- Dimensionless (reduced units)
- Thermophysical properties of the Lennard-Jones substance
- Mixtures of Lennard-Jones substances
- Equations of state for the Lennard-Jones potential
- Long-range interactions of the Lennard-Jones potential
- Lennard-Jones truncated & shifted (LJTS) potential
- Extensions and modifications of the Lennard-Jones potential
- See also
- References

Computational physics |
---|

Mechanics · Electromagnetics · Thermodynamics · Simulation |

The **Lennard-Jones potential** (also termed the **LJ potential** or **12-6 potential**) is an intermolecular pair potential. Among the intermolecular potentials, the Lennard-Jones potential is the potential that has been studied most extensively and most thoroughly. It is considered an archetype model for simple yet realistic intermolecular interactions.

The Lennard-Jones potential models soft repulsive and attractive interactions. Hence, the Lennard-Jones potential describes electronically neutral atoms or molecules. It is named after John Lennard-Jones.^{[1]}^{[2]}^{[3]} The commonly used expression for the Lennard-Jones potential is

where is the distance between two interacting particles, is the depth of the potential well (usually referred to as 'dispersion energy'), and is the distance at which the particle-particle potential energy is zero (often referred to as 'size of the particle'). The Lennard-Jones potential has its minimum at a distance of , where the potential energy has the value .

The Lennard-Jones potential is a simplified model that yet describes the essential features of interactions between simple atoms and molecules: Two interacting particles repel each other at very close distance, attract each other at moderate distance, and do not interact at infinite distance, see figure 1. The Lennard-Jones potential is a pair potential, i.e. no three- or multi-body interactions are covered by the potential.

Statistical mechanics^{[4]} and computer simulations^{[5]}^{[6]} can be used to study the Lennard-Jones potential and to obtain thermophysical properties of the 'Lennard-Jones substance'. Both the Lennard-Jones potential and, accordingly, the Lennard-Jones substance are simplified yet realistic models, such as they accurately capture essential physical principles like the presence of a critical and a triple point, condensation and freezing. The Lennard-Jones potential is mathematically simple and is therefore extensively used in studies on matter since the early days of computer simulation.^{[7]}^{[8]}^{[9]}^{[10]} Due to its mathematical simplicity and generic modeling capabilities, the Lennard-Jones potential is probably still the most frequently studied model potential.^{[11]}^{[12]} The Lennard-Jones substance is often even referred to as 'Lennard-Jonesium', suggesting that it is viewed as a chemical element. The Lennard-Jones potential is usually the standard choice for the development of theories for matter (especially soft-matter) as well as for the development and testing of computational methods and algorithms. Upon adjusting the model parameters and to real substance properties, the Lennard-Jones potential can be used to describe simple substance (like noble gases) with good accuracy. Furthermore, the Lennard-Jones potential is often used as a building block in molecular models (a.k.a. force fields) for more complex substances.^{[13]}^{[14]}^{[15]}^{[16]}^{[17]}

The Lennard-Jones potential models the two most important and fundamental molecular interactions: The repulsive term ( term) describes the Pauli repulsion at short distances of the interacting particles due to overlapping electron orbitals and the attractive term ( term) describes attraction at long ranged interactions (dispersion force), which vanish at infinite distance between two particles. The steep repulsive interactions at short distances yield the low compressibility of the solid and liquid phase; the attractive dispersive interactions act stabilizing for the condensed phase, especially the vapor-liquid equilibrium.

The functional form of the attractive term, the exponent '6', has a physical justification, which does not hold as rigorously for the repulsive term with the exponent '12'. The attractive dispersive interactions between simple atoms and molecules are a result of fluctuating partial charges. It has been shown by quantum-chemical calculations that this dispersive contribution has to decay with .^{[18]}

The term is mainly used because it can be implemented computationally very efficiently as the square of , which does not hold to the same extent for values other than '12'. Also, approximates the Pauli repulsion reasonably well. The Lennard-Jones potential can be generalized using arbitrary exponents instead of 12 and 6. The resulting potential is called Mie potential. The present article exclusively discusses the classical (12-6) Lennard-Jones potential.

The Lennard-Jones potential exhibits a pole at , i.e. the potential energy diverges to , which can cause instabilities in molecular simulations, e.g. for the sampling of the chemical potential. The Lennard-Jones potential converges to for . Hence, from a mathematical standpoint, attractive interactions stay present for infinitely distanced particles. These dispersive 'long-range' interactions have an important influence on several properties of the Lennard-Jones substance, e.g. the pressure or heat capacity in the vicinity of the critical point and the critical point itself. The importance of the long-range interactions were noticed already in the early stages of statistical mechanics.^{[19]} For computer simulations, only finite numbers of particles can be used, which leads to the fact that the potential can only be evaluated up to a finite radius , which is a so-called finite size effect. There are well-established methods to implicitly consider the thereby neglected long-range contribution for a given observable (details are given below).

It is often claimed that multiple Lennard-Jones potentials and corresponding substances exist depending on the handling of the long-range interactions. This is misleading. There is only one 'Lennard-Jones potential', which is exactly defined by Eq. (1). The Lennard-Jones potential requires the consideration and evaluation of long-range interactions up to very long (actually infinite) distances – at least so that the influence of the truncation has no influence on the observable of interest for the reported decimal places.

The Lennard-Jones potential implies that the particles are point masses with a mass . Even though the parameter is often referred to as 'size of the particle', particles interacting with the Lennard-Jones potential have no uniquely defined 'size' – opposite to the hard sphere potential. Particles interacting with the Lennard-Jones potential rather have soft repulsive cores.

The Lennard-Jones model describes the potential intermolecular energy between two particles based on the outlined principles. Following Newton's mechanics, the actual force between two interacting particles is simply obtained by negating and differentiating the Lennard-Jones potential with respect to , i.e. . Depending on the distance between the two particles, the net force can be either attractive or repulsive.

The Lennard-Jones potential yields a good approximation of intermolecular interactions for many applications: The macroscopic properties computed using the Lennard-Jones potential are in good agreement with experimental data for simple substances like argon on one side and the potential function is in fair agreement with results from quantum chemistry on the other side. The Lennard-Jones potential gives a good description of molecular interactions in fluid phases, whereas molecular interactions in solid phases are only roughly well described. This is mainly due to the fact that multi-body interactions play a significant role in solid phases, which are not comprised in the Lennard-Jones potential. Therefore, the Lennard-Jones potential is extensively used in soft-matter physics and associated fields, whereas it is less frequently used in solid-state physics. Due to its simplicity, the Lennard-Jones potential is often used to describe the properties of gases and simple fluids and to model dispersive and repulsive interactions in molecular models. It is especially accurate for noble gas atoms and methane. It is furthermore a good approximation for molecular interactions at long and short distances for neutral atoms and molecules. Therefore, the Lennard-Jones potential is very often used as a building block of molecular models of complex molecules, e.g. alkanes or water.^{[16]}^{[20]}^{[15]} The Lennard-Jones potential can also be used to model the adsorption interactions at solid-fluid interfaces, i.e. physisorption or chemisorption.

It is well accepted, that the main limitations of the Lennard-Jones potential lie in the fact the potential is a pair potential (does not cover multi-body interactions) and that the exponent term is used for the repulsion. Results from quantum chemistry suggest that a higher exponent than 12 has to be used, i.e. a steeper potential. Furthermore, the Lennard-Jones potential has a limited flexibility, i.e. only the two model parameters and can be used for the fitting to describe a real substance.

Numerous intermolecular potentials have been proposed in the past for the modeling of simple soft repulsive and attractive interactions between spherically symmetric particles, i.e. the general shape shown in figure 1. Examples for other potentials are the Morse potential, the Mie potential,^{[21]} the Buckingham potential and the Tang-Tönnies potential.^{[22]} Nevertheless, none of those are of such general importance as the Lennard-Jones potential.

The Lennard-Jones potential is not only of fundamental importance in computational chemistry and soft-matter physics, but also for the modeling of real substances. There are essentially two ways the Lennard-Jones potential can be used for that purpose: (1) A real substance atom or molecule is modeled directly by the Lennard-Jones potential, which yields very good results for noble gases and methane, i.e. dispersively interacting spherical particles. In the case of methane, the molecule is assumed to be spherically symmetric and the hydrogen atoms are fused with the carbon atom to a common unit. This simplification can in general also be applied to more complex molecules, but yields usually poor results. (2) A real substance molecule is built of multiple Lennard-Jones interactions sites, which can be connected either by rigid bonds or flexible additional potentials (and eventually also consists of other potential types, e.g. partial charges). Molecular models (often referred to as 'force fields') for practically all molecular and ionic particles can be constructed using this scheme for example for alkanes.

Upon using the first outlined approach, the molecular model has only the two parameters of the Lennard-Jones potential and that can be used for the fitting, e.g. and are frequently used for argon. Evidently, this approach is only a good approximation for spherical and simply dispersively interacting molecules and atoms. The direct use of the Lennard-Jones potential has the great advantage that simulation results and theories for the Lennard-Jones potential can be used directly. Hence, available results for the Lennard-Jones potential and substance can be directly scaled using the appropriate and (see reduced units). The Lennard-Jones potential parameters and can in general be fitted to any desired real substance property. In soft-matter physics, usually experimental data for the vapor-liquid phase equilibrium or the critical point is used for the parametrization; in solid-state physics, rather the compressibility, heat capacity or lattice constants are employed.^{[23]}^{[24]}

The second outlined approach of using the Lennard-Jones potential as a building block of elongated and complex molecules is far more sophisticated. Molecular models are thereby tailor-made in a sense that simulation results are only applicable for that particular model. This development approach for molecular force fields is today mainly performed in soft-matter physics and associated fields such as chemical engineering. A large number of force fields are based on the Lennard-Jones potential, e.g. the TraPPE force field,^{[16]} the OPLS force field,^{[25]} and the MolMod force field^{[15]} (an overview of molecular force fields is out of the scope of the present article). For the state-of-the-art modeling of solid-state materials, more elaborate multi-body potentials (e.g. EAM potentials^{[26]}) are used.

There are several different ways to formulate the Lennard-Jones potential besides Eq. (1). Alternatives are:

**AB form**

The AB form is frequently used in implementations of simulation software as it is computationally favorable. The Lennard-Jones potential can be written as

where, and . Conversely, and . This is the form in which Lennard-Jones wrote the potential named after him.^{[27]}

**n-exp form**

The n-exp form is a mathematically more general form and can be written as

where is the bonding energy of the molecule (the energy required to separate the atoms). Applying an harmonic approximation at the potential minimum (at ), the exponent and the energy parameter can be related to the spring constant:

from where can be calculated if is known. Normally the harmonic states are known, , where . * can also be related to the group velocity in a crystal,
*

where * is the lattice distance, and is the mass of a particle.
*

Property | Symbol | Reduced form |
---|---|---|

Length | ||

Time | ||

Temperature | ||

Force | ||

Energy | ||

Pressure | ||

Density | ||

Surface tension |

Dimensionless reduced units can be defined based on the Lennard-Jones potential parameters, which is convenient for molecular simulations. From a numerical point of view, the advantages of this unit system include computing values which are closer to unity, using simplified equations and being able to easily scale the results.^{[28]}^{[5]} This reduced units system requires the specification of the size parameter and the energy parameter of the Lennard-Jones potential and the mass of the particle . All physical properties can be converted straightforwardly taking the respective dimension into account, see table. The reduced units are often abbreviated and indicated by an asterisk.

In general, reduced units can also be built up on other molecular interaction potentials that consist of a length parameter and an energy parameter.

Thermophysical properties of the Lennard-Jones substance, i.e. particles interacting with the Lennard-Jones potential can be obtained using statistical mechanics. Some properties can be computed analytically, i.e. with machine precision, whereas most properties can only be obtained by performing molecular simulations.^{[5]} The latter will in general be superimposed by both statistical and systematic uncertainties.^{[31]}^{[12]}^{[32]}^{[33]} The virial coefficients can for example be computed directly from the Lennard-potential using algebraic expressions^{[4]} and reported data has therefore no uncertainty. Molecular simulation results, e.g. the pressure at a given temperature and density has both statistical and systematic uncertainties.^{[31]}^{[33]} Molecular simulations of the Lennard-Jones potential can in general be performed using either molecular dynamics (MD) simulations or Monte Carlo (MC) simulation. For MC simulations, the Lennard-Jones potential is directly used, whereas MD simulations are always based on the derivative of the potential, i.e. the force . These differences in combination with differences in the treatment of the long-range interactions (see below) can influence computed thermophysical properties.^{[34]}^{[35]}

Since the *Lennard-Jonesium* is the archetype for the modeling of simple yet realistic intermolecular interactions, a large number of thermophysical properties were studied and reported in the literature.^{[12]} Computer experiment data of the Lennard-Jones potential is presently considered the most accurately known data in classical mechanics computational chemistry. Hence, such data is also mostly used as benchmark for the validation and testing of new algorithms and theories. The Lennard-Jones potential has been constantly used since the early days of molecular simulations. The first results from computer experiments for the Lennard-Jones potential were reported by Rosenbluth and Rosenbluth^{[8]} and Wood and Parker^{[7]} after molecular simulations on "fast computing machines" became available in 1953.^{[36]} Since then many studies reported data of the Lennard-Jones substance;^{[12]} approximately 50,000 data points are publicly available. The current state of research of thermophysical properties of the Lennard-Jones substance is summarized in the following. The most comprehensive summary and digital database was given by Stephan et al.^{[12]} Presently, no data repository covers and maintains this database (or any other model potential) – even data and results stated by the NIST website should be treated with caution (not reproducible and misleading referencing^{[12]}).

Figure 2 shows the phase diagram of the Lennard-Jones fluid. Phase equilibria of the Lennard-Jones potential have been studied numerous times and are accordingly known today with good precision.^{[29]}^{[12]}^{[37]} Figure 2 shows results correlations derived from computer experiment results (hence, lines instead of data points are shown).

The mean intermolecular interaction of a Lennard-Jones particle strongly depends on the thermodynamic state, i.e. temperature and pressure (or density). For solid states, the attractive Lennard-Jones interaction plays a dominant role – especially at low temperatures. For liquid states, no ordered structure is present compared to solid states. The mean potential energy per particle is negative. For gaseous states, attractive interactions of the Lennard-Jones potential play a minor role – since they are far distanced. The main part of the internal energy is stored as kinetic energy for gaseous states. At supercritical states, the attractive Lennard-Jones interaction plays a minor role. With increasing temperature, the mean kinetic energy of the particles increases and exceeds the energy well of the Lennard-Jones potential. Hence, the particles mainly interact by the potentials' soft repulsive interactions and the mean potential energy per particle is accordingly positive.

Overall, due to the large timespan the Lennard-Jones potential has been studied and thermophysical property data has been reported in the literature and computational resources were insufficient for accurate simulations (to modern standards), a noticeable amount of data is known to be dubious.^{[12]} Nevertheless, in many studies dodge data is used as reference. The lack of data repositories and data assessment is a crucial element for future work in the long-going field of Lennard-Jones potential research.

The most important characteristic points of the Lennard-Jones potential are the critical point and the vapor-liquid-solid triple point. They were studied numerous times in the literature and compiled in Ref.^{[12]} The critical point was thereby assessed to be located at

The given uncertainties were calculated from the standard deviation of the critical parameters derived from the most reliable available vapor-liquid equilibrium data sets.^{[12]} These uncertainties can be assumed as a lower limit to the accuracy with which the critical point of fluid can be obtained from molecular simulation results.

The triple point is presently assumed to be located at

The uncertainties represent the scattering of data from different authors.^{[29]} The critical point of the Lennard-Jones substance has been studied far more often than the triple point. For both the critical point and the vapor-liquid-solid triple point, several studies reported results out of the above stated ranges. The above stated data is the presently assumed correct and reliable data. Nevertheless, the determinateness of the critical temperature and the triple point temperature is still unsatisfactory.

Evidently, the phase coexistence curves (cf. figure 2) are of fundamental importance to characterize the Lennard-Jones potential. Furthermore, *Brown's characteristic curves*^{[41]} yield an illustrative description of essential features of the Lennard-Jones potential. Brown's characteristic curves are defined as curves on which a certain thermodynamic property of the substance matches that of an ideal gas. For a real fluid, and its derivatives can match the values of the ideal gas for special , combinations only as a result of Gibbs' phase rule. The resulting points collectively constitute a characteristic curve. Four main characteristic curves are defined: One 0th-order (named *Zeno curve*) and three 1st-order curves (named *Amagat*, *Boyle*, and *Charles curve*). The characteristic curve are required to have a negative or zero curvature throughout and a single maximum in a double-logarithmic pressure-temperature diagram. Furthermore, Brown's characteristic curves and the virial coefficients are directly linked in the limit of the ideal gas and are therefore known exactly at . Both computer simulation results and equation of state results have been reported in the literature for the Lennard-Jones potential.^{[39]}^{[12]}^{[38]}^{[42]}^{[43]}

Points on the Zeno curve Z have a compressibility factor of unity . The Zeno curve originates at the Boyle temperature , surrounds the critical point, and has a slope of unity in the low temperature limit.^{[38]} Points on the Boyle curve B have . The Boyle curve originates with the Zeno curve at the Boyle temperature, faintly surrounds the critical point, and ends on the vapor pressure curve. Points on the Charles curve (a.k.a. Joule-Thomson inversion curve) have and more importantly , i.e. no temperature change upon isenthalpic throttling. It originates at in the ideal gas limit, crosses the Zeno curve, and terminates on the vapor pressure curve. Points on the Amagat curve A have . It also starts in the ideal gas limit at , surrounds the critical point and the other three characteristic curves and passes into the solid phase region. A comprehensive discussion of the characteristic curves of the Lennard-Jones potential is given by Stephan and Deiters.^{[38]}

Properties of the Lennard-Jones fluid have been studied extensively in the literature due to the outstanding importance of the Lennard-Jones potential in soft-matter physics and related fields. About 50 datasets of computer experiment data for the vapor-liquid equilibrium have been published to date.^{[12]} Furthermore, more than 35,000 data points at homogeneous fluid states have been published over the years and recently been compiled and assessed for outliers in an open access database.^{[12]}

The vapor-liquid equilibrium of the Lennard-Jones substance is presently known with a precision, i.e. mutual agreement of thermodynamically consistent data, of for the vapor pressure, for the saturated liquid density, for the saturated vapor density, for the enthalpy of vaporization, and for the surface tension.^{[12]} This status quo can not be considered satisfactory considering the fact that statistical uncertainties usually reported for single data sets are significantly below the above stated values (even for far more complex molecular force fields).

Both phase equilibrium properties and homogeneous state properties at arbitrary density can in general only be obtained from molecular simulations, whereas virial coefficients can be computed directly from the Lennard-Jones potential.^{[4]} Numerical data for the second and third virial coefficient is available in a wide temperature range.^{[45]}^{[38]}^{[12]} For higher virial coefficients (up to the sixteenth), the number of available data points decreases with increasing number of the virial coefficient.^{[46]}^{[47]} Also transport properties (viscosity, heat conductivity, and self diffusion coefficient) of the Lennard-Jones fluid have been studied frequently,^{[48]}^{[49]} but the database is significantly less dense than for homogeneous equilibrium properties like – or internal energy data. Moreover, a large number of analytical models (equations of state) have been developed for the description of the Lennard-Jones fluid (see below for details).

The database and knowledge for the Lennard-Jones solid is significantly poorer than for the fluid phases, which is mainly due to the fact that the Lennard-Jones potential is less frequently used in applications for the modeling of solid substances. It was realized early that the interactions in solid phases should not be approximated to be pair-wise additive – especially for metals.^{[23]}^{[24]}

Nevertheless, the Lennard-Jones potential is still frequently used in solid-state physics due to its simplicity and computational efficiency. Hence, the basic properties of the solid phases and the solid-fluid phase equilibria have been investigated several times, e.g. Refs.^{[37]}^{[29]}^{[30]}^{[50]}^{[51]}^{[40]}

The Lennard-Jones substance form fcc (face centered cubic), hcp (hexagonal close-packed) and other close-packed polytype lattices – depending on temperature and pressure, cf. figure 2. At low temperature and up to moderate pressure, the hcp lattice is energetically favored and therefore the equilibrium structure. The fcc lattice structure is energetically favored at both high temperature and high pressure and therefore overall the equilibrium structure in a wider state range. The coexistence line between the fcc and hcp phase starts at at approximately , passes through a temperature maximum at approximately , and then ends on the vapor-solid phase boundary at approximately , which thereby forms a triple point.^{[50]}^{[29]} Hence, only the fcc solid phase exhibits phase equilibria with the liquid and supercritical phase, cf. figure 2.

The triple point of the two solid phases (fcc and hcp) and the vapor phase is reported to be located at:^{[50]}^{[29]}

- not reported yet

Note, that other and significantly differing values have also been reported in the literature. Hence, the database for the fcc-hcp-vapor triple point should be further solidified in the future.

Mixtures of Lennard-Jones particles are mostly used as a prototype for the development of theories and methods of solutions, but also to study properties of solutions in general. This dates back to the fundamental work of conformal solution theory of Longuet-Higgins^{[52]} and Leland and Rowlinson and co-workers.^{[53]}^{[54]} Those are today the basis of most theories for mixtures.^{[55]}^{[56]}

Mixtures of two or more Lennard-Jones components are set up by changing at least one potential interaction parameter ( or ) of one of the components with respect to the other. For a binary mixture, this yields three types of pair interactions that are all modeled by the Lennard-Jones potential: 1-1, 2-2, and 1-2 interactions. For the cross interactions 1-2, additional assumptions are required for the specification of parameters or from , and , . Various choices (all more or less empirical and not rigorously based on physical arguments) can be used for these co-called combination rules.^{[57]} The by far most frequently used combination rule is the one of Lorentz and Berthelot^{[58]}

The parameter is an additional state-independent interaction parameter for the mixture. The parameter is usually set to unity since the arithmetic mean can be considered physically plausible for the cross-interaction size parameter. The parameter on the other hand is often used to adjust the phase behavior of the model mixture. For analytical models, e.g. equations of state, the deviation parameter is usually written as . For , the cross-interaction dispersion energy and accordingly the attractive force between unlike particles is intensified. Vice versa, the attractive forces between unlike particles are diminished for .

For Lennard-Jones mixtures, both fluid and solid phase equilibria can be studied, i.e. vapor-liquid, liquid-liquid, gas-gas, solid-vapor, solid-liquid, and solid-solid. Accordingly, different types of triple points (three-phase equilibria) and critical points can exist as well as different eutectic and azeotropic points.^{[59]}^{[56]} Binary Lennard-Jones mixtures in the fluid region (various types of equilibria of liquid and gas phases)^{[44]}^{[60]}^{[61]}^{[62]}^{[63]} have been studied more comprehensively then phase equilibria comprising solid phases.^{[64]}^{[65]}^{[66]}^{[67]}^{[68]} A large number of different Lennard-Jones mixtures have been studied in the literature. To date, no standard for such has been established. Usually, the binary interaction parameters and the two component parameters are chosen such that a mixture with properties convenient for a given task are obtained. Yet, this makes comparisons often tricky.

For the fluid phase behavior, mixtures exhibit practically ideal behavior (in the sense of Raoult's law) for . For attractive interactions prevail and the mixtures tend to form high-boiling azeotropes, i.e. a lower pressure than pure components' vapor pressures is required to stabilize the vapor-liquid equilibrium. For repulsive interactions prevail and mixtures tend to form low-boiling azeotropes, i.e. a higher pressure than pure components' vapor pressures is required to stabilize the vapor-liquid equilibrium since the mean dispersive forces are decreased. Particularly low values of furthermore will result in liquid-liquid miscibility gaps. Also various types of phase equilibria comprising solid phases have been studied in the literature, e.g. by Carol and co-workers.^{[66]}^{[68]}^{[65]}^{[64]} Also, cases exist where the solid phase boundaries interrupt fluid phase equilibria. However, for phase equilibria that comprise solid phases, the amount of published data is sparse.

A large number equations of state (EOS) for the Lennard-Jones potential/ substance have been proposed since its characterization became available with the first computer simulations.^{[36]} Due to the fundamental importance of the Lennard-Jones potential, most currently available EOS describe the Lennard-Jones fluid. They have been comprehensively reviewed by Stephan et al.^{[11]}^{[38]}

Equations of state for the Lennard-Jones fluid are of particular importance in soft-matter physics and physical chemistry since those are frequently used as starting point for the development of EOS for complex fluids, e.g. polymers and associating fluids. The monomer units of these models are usually directly adapted from Lennard-Jones EOS as a building block, e.g. the PHC EOS,^{[69]} the BACKONE EOS,^{[70]}^{[71]} and SAFT type EOS.^{[72]}^{[73]}^{[74]}^{[75]}

More than 30 Lennard-Jones EOS have been proposed in the literature. A comprehensive evaluation^{[11]}^{[38]} of such EOS showed that several EOS^{[76]}^{[77]}^{[78]}^{[79]} describe the Lennard-Jones potential with good and similar accuracy, but none of them is outstanding. Three of those EOS show an unacceptable unphysical behavior in some fluid region, e.g. multiple van der Waals loops, while being elsewise reasonably precise. Only the Lennard-Jones EOS of Kolafa and Nezbeda^{[77]} was found to be robust and precise for most thermodynamic properties of the Lennard-Jones fluid.^{[38]}^{[11]} Hence, the Lennard-Jones EOS of Kolafa and Nezbeda^{[77]} is presently considered to be most useful choice – because robust and precise. Furthermore, the Lennard-Jones EOS of Johnson et al.^{[80]} was found to be less precise for practically all available reference data^{[12]}^{[11]} than the Kolafa and Nezbeda EOS.^{[77]} It is interesting to note that the LJ EOS Johnson et al.^{[80]} is yet far more often used than that of Kolafa and Nezbeda.^{[77]}

The Lennard-Jones potential, cf. Eq. (1) and figure 1, has an infinite range. Only under its consideration, the 'true' and 'full' Lennard-Jones potential is examined. For the evaluation of an observable of an ensemble of particles interacting by the Lennard-Jones potential using molecular simulations, the interactions can only be evaluated explicitly up to a certain distance – simply due to the fact that the number of particles will always be finite. The maximum distance applied in a simulation is usually referred to as 'cut-off' radius (because the Lennard-Jones potential is radially symmetric). To obtain thermophysical properties (both macroscopic or microscopic) of the 'true' and 'full' Lennard-Jones (LJ) potential, the contribution of the potential beyond the cut-off radius has to be accounted for.

Different corrections schemes have been developed to account for the influence of the long-range interactions in simulations and to sustain a sufficiently good approximation of the 'full' potential.^{[6]}^{[28]} They are based on simplifying assumptions regarding the structure of the fluid. For simple cases, such as in studies of the equilibrium of homogeneous fluids, simple correction terms yield excellent results. In other cases, such as in studies of inhomogeneous systems with different phases, accounting for the long-range interactions is more tedious. These corrections are usually referred to as 'long-range corrections'. For most properties, simple analytical expressions are known and well established. For a given observable , the 'corrected' simulation result is then simply computed from the actually sampled value and the long-range correction value , e.g. for the internal energy .^{[28]} The hypothetical true value of the observable of the Lennard-Jones potential at truly infinite cut-off distance (thermodynamic limit) can in general only be estimated.

Furthermore, the quality of the long-range correction scheme depends on the cut-off radius. The assumptions made with the correction schemes are usually not justified at (very) short cut-off radii. This is illustrated in the example shown in figure 7. The long-range correction scheme is said to be converged, if the remaining error of the correction scheme is sufficiently small at a given cut-off distance, cf. figure 7.

The Lennard-Jones truncated & shifted (LJTS) potential is an often used alternative to the 'full' Lennard-Jones potential (see Eq. (1)). The 'full' and the 'truncated & shifted' Lennard-Jones potential have to be kept strictly separate. They are simply two different potentials yielding different thermophysical properties. The Lennard-Jones truncated & shifted potential is defined as

with

Hence, the LJTS potential is sturdily truncated at and shifted by the corresponding energy value . The latter is applied to avoid a discontinuity jump of the potential at . For the LJTS potential, no long-range interactions beyond are considered – neither explicitly nor implicitly. The potential simply ends abruptly at . The most frequently used version of the Lennard-Jones truncated & shifted potential is the one with . Nevertheless, different values have been used in the literature.^{[83]}^{[84]}^{[85]}^{[86]} Each LJTS potential with a given truncation radius has to be considered as a potential and accordingly a substance of its own.

The LJTS potential is computationally significantly cheaper than the 'full' Lennard-Jones potential, but still covers the essential physical features of matter (the presence of a critical and a triple point, soft repulsive and attractive interactions, phase equilibria etc.). Therefore, the LJTS potential is very frequently used for the testing of new algorithms, simulation methods, and new physical theories.^{[87]}^{[88]}^{[89]}^{[90]}

Interestingly, for homogeneous systems, the intermolecular forces that are calculated from the LJ and the LJTS potential at a given distance are the same (since is the same), whereas the potential energy and the pressure are affected by the shifting. Also, the properties of the LJTS substance may furthermore be affected by the chosen simulation algorithm, i.e. MD or MC sampling (this is in general not the case for the 'full' Lennard-Jones potential).

For the LJTS potential with , the potential energy shift is approximately 1/60 of the dispersion energy at the potential well: . The figure 8 shows the comparison of the vapor-liquid equilibrium of the 'full' Lennard-Jones potential and the 'Lennard-Jones truncated & shifted' potential. The 'full' Lennard-Jones potential results prevail a significantly higher critical temperature and pressure compared to the LJTS potential results, but the critical density is very similar.^{[44]}^{[35]}^{[85]} The vapor pressure and the enthalpy of vaporization are influenced more strongly by the long-range interactions than the saturated densities. This is due to the fact that the potential is manipulated mainly energetically by the truncation and shifting.

The Lennard-Jones potential – as archetype for intermolecular potentials – has been used numerous times as starting point for the development of more elaborated intermolecular potentials. Various extension and modifications of the Lennard-Jones potential have been proposed in the literature. One could argue that all force fields (hundreds exists) can be traced back to the Lennard-Jones potential. A more extensive list is given in the 'interatomic potential' functions article. The following list refers only to potentials that are directly related to the Lennard-Jones potential and are of both historic importance and still relevant for present research

**Mie potential**The Mie potential is the generalized version of the Lennard-Jones potential, i.e. the exponents 12 and 6 are introduced as parameters and . Especially thermodynamic derivative properties, e.g. the compressibility and the speed of sound, are known to be very sensitive to the steepness of the repulsive part of the intermolecular potential, which can therefore be modeled more sophisticated by the Mie potential.^{[72]}The first explicit formulation of the Mie potential is attributed to Eduard Grüneisen.^{[91]}^{[92]}Hence, the Mie potential was actually proposed before the Lennard-Jones potential. The Mie potential is named after Gustav Mie.^{[21]}**Buckingham potential**The Buckingham potential was proposed by Richard Buckingham. The repulsive part of the Lennard-Jones potential is therein replaced by an exponential function and it incorporates an additional parameter.**Stockmayer potential**The Stockmayer potential is named after W.H. Stockmayer.^{[93]}The Stockmayer potential is a combination of a Lennard-Jones potential superimposed by a dipole. Hence, Stockmayer particles are not spherically symmetric, but rather have an important orientational structure.**Two center Lennard-Jones potential**The two center Lennard-Jones potential consists of two identical Lennard-Jones interaction sites (same , , ) that are bonded as a rigid body. It is often abbreviated as 2CLJ. Usually, the elongation (distance between the Lennard-Jones sites) is significantly smaller than the size parameter . Hence, the two interaction sites are significantly fused.**Lennard-Jones truncated & splined potential**The Lennard-Jones truncated & splined potential is a rarely used yet useful potential. Similar to the more popular LJTS potential, it is sturdily truncated at a certain 'end' distance and no long-range interactions are considered beyond. Opposite to the LJTS potential, which is shifted such that the potential is continuous, the Lennard-Jones truncated & splined potential is made continuous by using an arbitrary but favorable spline function.

Wikimedia Commons has media related to Lennard-Jones potentials. |

**^**Jones, J. E. (1924). "On the determination of molecular fields.—I. From the variation of the viscosity of a gas with temperature".*Proceedings of the Royal Society of London. Series A, Containing Papers of a Mathematical and Physical Character*.**106**(738): 441–462. Bibcode:1924RSPSA.106..441J. doi:10.1098/rspa.1924.0081. ISSN 0950-1207.**^**Jones, J. E. (1924). "On the determination of molecular fields. —II. From the equation of state of a gas".*Proceedings of the Royal Society of London. Series A, Containing Papers of a Mathematical and Physical Character*.**106**(738): 463–477. Bibcode:1924RSPSA.106..463J. doi:10.1098/rspa.1924.0082. ISSN 0950-1207.**^**Lennard-Jones, J E (1931-09-01). "Cohesion".*Proceedings of the Physical Society*.**43**(5): 461–482. Bibcode:1931PPS....43..461L. doi:10.1088/0959-5309/43/5/301. ISSN 0959-5309.- ^
^{a}^{b}^{c}Hill, Terrell L. (1956).*Statistical mechanics : principles and selected applications*. New York: Dover Publications. ISBN 0-486-65390-0. OCLC 15163657. - ^
^{a}^{b}^{c}D. C. Rapaport (1 April 2004).*The Art of Molecular Dynamics Simulation*. Cambridge University Press. ISBN 978-0-521-82568-9. - ^
^{a}^{b}Frenkel, D.; Smit, B. (2002),*Understanding Molecular Simulation*(Second ed.), San Diego: Academic Press, ISBN 0-12-267351-4 - ^
^{a}^{b}Wood, W. W.; Parker, F. R. (1957). "Monte Carlo Equation of State of Molecules Interacting with the Lennard‐Jones Potential. I. A Supercritical Isotherm at about Twice the Critical Temperature".*The Journal of Chemical Physics*.**27**(3): 720–733. Bibcode:1957JChPh..27..720W. doi:10.1063/1.1743822. ISSN 0021-9606. - ^
^{a}^{b}Rosenbluth, Marshall N.; Rosenbluth, Arianna W. (1954). "Further Results on Monte Carlo Equations of State".*The Journal of Chemical Physics*.**22**(5): 881–884. Bibcode:1954JChPh..22..881R. doi:10.1063/1.1740207. ISSN 0021-9606. **^**Alder, B. J.; Wainwright, T. E. (1959). "Studies in Molecular Dynamics. I. General Method".*The Journal of Chemical Physics*.**31**(2): 459–466. Bibcode:1959JChPh..31..459A. doi:10.1063/1.1730376. ISSN 0021-9606.**^**Rahman, A. (1964-10-19). "Correlations in the Motion of Atoms in Liquid Argon".*Physical Review*.**136**(2A): A405–A411. Bibcode:1964PhRv..136..405R. doi:10.1103/PhysRev.136.A405. ISSN 0031-899X.- ^
^{a}^{b}^{c}^{d}^{e}^{f}^{g}^{h}^{i}Stephan, Simon; Staubach, Jens; Hasse, Hans (2020). "Review and comparison of equations of state for the Lennard-Jones fluid".*Fluid Phase Equilibria*.**523**: 112772. doi:10.1016/j.fluid.2020.112772. S2CID 224844789. - ^
^{a}^{b}^{c}^{d}^{e}^{f}^{g}^{h}^{i}^{j}^{k}^{l}^{m}^{n}^{o}^{p}^{q}^{r}^{s}^{t}^{u}Stephan, Simon; Thol, Monika; Vrabec, Jadran; Hasse, Hans (2019-10-28). "Thermophysical Properties of the Lennard-Jones Fluid: Database and Data Assessment".*Journal of Chemical Information and Modeling*.**59**(10): 4248–4265. doi:10.1021/acs.jcim.9b00620. ISSN 1549-9596. PMID 31609113. S2CID 204545481. **^**Jorgensen, William L.; Maxwell, David S.; Tirado-Rives, Julian (January 1996). "Development and Testing of the OPLS All-Atom Force Field on Conformational Energetics and Properties of Organic Liquids".*Journal of the American Chemical Society*.**118**(45): 11225–11236. doi:10.1021/ja9621760. ISSN 0002-7863.**^**Wang, Junmei; Wolf, Romain M.; Caldwell, James W.; Kollman, Peter A.; Case, David A. (2004-07-15). "Development and testing of a general amber force field".*Journal of Computational Chemistry*.**25**(9): 1157–1174. doi:10.1002/jcc.20035. ISSN 0192-8651. PMID 15116359. S2CID 18734898.- ^
^{a}^{b}^{c}Stephan, Simon; Horsch, Martin T.; Vrabec, Jadran; Hasse, Hans (2019-07-03). "MolMod – an open access database of force fields for molecular simulations of fluids".*Molecular Simulation*.**45**(10): 806–814. arXiv:1904.05206. doi:10.1080/08927022.2019.1601191. ISSN 0892-7022. S2CID 119199372. - ^
^{a}^{b}^{c}Eggimann, Becky L.; Sunnarborg, Amara J.; Stern, Hudson D.; Bliss, Andrew P.; Siepmann, J. Ilja (2014-01-02). "An online parameter and property database for the TraPPE force field".*Molecular Simulation*.**40**(1–3): 101–105. doi:10.1080/08927022.2013.842994. ISSN 0892-7022. S2CID 95716947. **^**Zhen, Shu; Davies, G. J. (16 August 1983). "Calculation of the Lennard-Jones*n*–*m*potential energy parameters for metals".*Physica Status Solidi A*.**78**(2): 595–605. Bibcode:1983PSSAR..78..595Z. doi:10.1002/pssa.2210780226.**^**Eisenschitz, R.; London, F. (1930-07-01). "Über das Verhältnis der van der Waalsschen Kräfte zu den homöopolaren Bindungskräften".*Zeitschrift für Physik*(in German).**60**(7): 491–527. Bibcode:1930ZPhy...60..491E. doi:10.1007/BF01341258. ISSN 0044-3328. S2CID 125644826.**^**Rowlinson, J. S. (2006-11-20). "The evolution of some statistical mechanical ideas".*Molecular Physics*.**104**(22–24): 3399–3410. Bibcode:2006MolPh.104.3399R. doi:10.1080/00268970600965835. ISSN 0026-8976. S2CID 119942778.**^**Abascal, J. L. F.; Vega, C. (2005-12-15). "A general purpose model for the condensed phases of water: TIP4P/2005".*The Journal of Chemical Physics*.**123**(23): 234505. Bibcode:2005JChPh.123w4505A. doi:10.1063/1.2121687. ISSN 0021-9606. PMID 16392929.- ^
^{a}^{b}Mie, Gustav (1903). "Zur kinetischen Theorie der einatomigen Körper".*Annalen der Physik*(in German).**316**(8): 657–697. Bibcode:1903AnP...316..657M. doi:10.1002/andp.19033160802. **^**Tang, K. T.; Toennies, J. Peter (1984-04-15). "An improved simple model for the van der Waals potential based on universal damping functions for the dispersion coefficients".*The Journal of Chemical Physics*.**80**(8): 3726–3741. Bibcode:1984JChPh..80.3726T. doi:10.1063/1.447150. ISSN 0021-9606.- ^
^{a}^{b}Zhen, Shu; Davies, G. J. (1983-08-16). "Calculation of the Lennard-Jonesn–m potential energy parameters for metals".*Physica Status Solidi A*(in German).**78**(2): 595–605. Bibcode:1983PSSAR..78..595Z. doi:10.1002/pssa.2210780226. - ^
^{a}^{b}Halicioglu, T.; Pound, G. M. (1975-08-16). "Calculation of potential energy parameters form crystalline state properties".*Physica Status Solidi A*.**30**(2): 619–623. Bibcode:1975PSSAR..30..619H. doi:10.1002/pssa.2210300223. **^**Jorgensen, William L.; Maxwell, David S.; Tirado-Rives, Julian (January 1996). "Development and Testing of the OPLS All-Atom Force Field on Conformational Energetics and Properties of Organic Liquids".*Journal of the American Chemical Society*.**118**(45): 11225–11236. doi:10.1021/ja9621760. ISSN 0002-7863.**^**Mendelev, M. I.; Han, S.; Srolovitz, D. J.; Ackland, G. J.; Sun, D. Y.; Asta, M. (2003). "Development of new interatomic potentials appropriate for crystalline and liquid iron".*Philosophical Magazine*.**83**(35): 3977–3994. Bibcode:2003PMag...83.3977A. doi:10.1080/14786430310001613264. ISSN 1478-6435. S2CID 4119718.**^**Lennard-Jones, J. E. (1931). "Cohesion".*Proceedings of the Physical Society*.**43**(5): 461–482. Bibcode:1931PPS....43..461L. doi:10.1088/0959-5309/43/5/301.- ^
^{a}^{b}^{c}Allen, Michael P.; Tildesley, Dominic J. (2017-11-23). "Computer Simulation of Liquids".*Oxford Scholarship Online*. doi:10.1093/oso/9780198803195.001.0001. ISBN 9780198803195. - ^
^{a}^{b}^{c}^{d}^{e}^{f}^{g}^{h}Schultz, Andrew J.; Kofke, David A. (2018-11-28). "Comprehensive high-precision high-accuracy equation of state and coexistence properties for classical Lennard-Jones crystals and low-temperature fluid phases".*The Journal of Chemical Physics*.**149**(20): 204508. doi:10.1063/1.5053714. ISSN 0021-9606. PMID 30501268. S2CID 54629914. - ^
^{a}^{b}Schultz, Andrew J.; Kofke, David A. (2020-08-07). "Erratum: "Comprehensive high-precision high-accuracy equation of state and coexistence properties for classical Lennard-Jones crystals and low-temperature fluid phases" [J. Chem. Phys. 149, 204508 (2018)]".*The Journal of Chemical Physics*.**153**(5): 059901. Bibcode:2020JChPh.153e9901S. doi:10.1063/5.0021283. ISSN 0021-9606. PMID 32770918. - ^
^{a}^{b}Schappals, Michael; Mecklenfeld, Andreas; Kröger, Leif; Botan, Vitalie; Köster, Andreas; Stephan, Simon; García, Edder J.; Rutkai, Gabor; Raabe, Gabriele; Klein, Peter; Leonhard, Kai (2017-09-12). "Round Robin Study: Molecular Simulation of Thermodynamic Properties from Models with Internal Degrees of Freedom".*Journal of Chemical Theory and Computation*.**13**(9): 4270–4280. doi:10.1021/acs.jctc.7b00489. ISSN 1549-9618. PMID 28738147. **^**Loeffler, Hannes H.; Bosisio, Stefano; Duarte Ramos Matos, Guilherme; Suh, Donghyuk; Roux, Benoit; Mobley, David L.; Michel, Julien (2018-11-13). "Reproducibility of Free Energy Calculations across Different Molecular Simulation Software Packages".*Journal of Chemical Theory and Computation*.**14**(11): 5567–5582. doi:10.1021/acs.jctc.8b00544. hdl:20.500.11820/52d85d71-d3df-468b-8f88-9c52e83da1f1. ISSN 1549-9618. PMID 30289712. S2CID 52923832.- ^
^{a}^{b}Lenhard, Johannes; Küster, Uwe (2019). "Reproducibility and the Concept of Numerical Solution".*Minds and Machines*.**29**(1): 19–36. doi:10.1007/s11023-019-09492-9. ISSN 0924-6495. S2CID 59159685. **^**Shi, Wei; Johnson, J. Karl (2001-09-15). "Histogram reweighting and finite-size scaling study of the Lennard–Jones fluids".*Fluid Phase Equilibria*. 187–188: 171–191. doi:10.1016/S0378-3812(01)00534-9. ISSN 0378-3812.- ^
^{a}^{b}Smit, B. (1992), "Phase diagrams of Lennard-Jones fluids" (PDF),*Journal of Chemical Physics*,**96**(11): 8639–8640, Bibcode:1992JChPh..96.8639S, doi:10.1063/1.462271 - ^
^{a}^{b}Metropolis, Nicholas; Rosenbluth, Arianna W.; Rosenbluth, Marshall N.; Teller, Augusta H.; Teller, Edward (1953). "Equation of State Calculations by Fast Computing Machines".*The Journal of Chemical Physics*.**21**(6): 1087–1092. Bibcode:1953JChPh..21.1087M. doi:10.1063/1.1699114. ISSN 0021-9606. OSTI 4390578. - ^
^{a}^{b}Köster, Andreas; Mausbach, Peter; Vrabec, Jadran (2017-10-10). "Premelting, solid-fluid equilibria, and thermodynamic properties in the high density region based on the Lennard-Jones potential".*The Journal of Chemical Physics*.**147**(14): 144502. Bibcode:2017JChPh.147n4502K. doi:10.1063/1.4990667. ISSN 0021-9606. PMID 29031254. - ^
^{a}^{b}^{c}^{d}^{e}^{f}^{g}^{h}^{i}Stephan, Simon; Deiters, Ulrich K. (2020-08-20). "Characteristic Curves of the Lennard-Jones Fluid".*International Journal of Thermophysics*.**41**(10): 147. Bibcode:2020IJT....41..147S. doi:10.1007/s10765-020-02721-9. ISSN 1572-9567. PMC 7441092. PMID 32863513. - ^
^{a}^{b}Deiters, Ulrich K.; Neumaier, Arnold (2016-08-11). "Computer Simulation of the Characteristic Curves of Pure Fluids".*Journal of Chemical & Engineering Data*.**61**(8): 2720–2728. doi:10.1021/acs.jced.6b00133. ISSN 0021-9568. - ^
^{a}^{b}Agrawal, Rupal; Kofke, David A. (1995). "Thermodynamic and structural properties of model systems at solid-fluid coexistence: II. Melting and sublimation of the Lennard-Jones system".*Molecular Physics*.**85**(1): 43–59. doi:10.1080/00268979500100921. ISSN 0026-8976. **^**Brown, E.H. (1960). "On the thermodynamic properties of fluids".*Bulletin de l'Institut International du Froid*. Annexe 1960-1: 169–178.**^**Apfelbaum, E. M.; Vorob’ev, V. S. (2020-06-18). "The Line of the Unit Compressibility Factor (Zeno-Line) for Crystal States".*The Journal of Physical Chemistry B*.**124**(24): 5021–5027. doi:10.1021/acs.jpcb.0c02749. ISSN 1520-6106. PMID 32437611. S2CID 218835048.**^**Apfelbaum, E. M.; Vorob’ev, V. S.; Martynov, G. A. (2008). "Regarding the Theory of the Zeno Line".*The Journal of Physical Chemistry A*.**112**(26): 6042–6044. Bibcode:2008JPCA..112.6042A. doi:10.1021/jp802999z. ISSN 1089-5639. PMID 18543889.- ^
^{a}^{b}^{c}^{d}^{e}Stephan, Simon; Hasse, Hans (2020-06-01). "Influence of dispersive long-range interactions on properties of vapour–liquid equilibria and interfaces of binary Lennard-Jones mixtures".*Molecular Physics*.**118**(9–10): e1699185. Bibcode:2020MolPh.11899185S. doi:10.1080/00268976.2019.1699185. ISSN 0026-8976. S2CID 214174102. **^**Nicolas, J.J.; Gubbins, K.E.; Streett, W.B.; Tildesley, D.J. (1979). "Equation of state for the Lennard-Jones fluid".*Molecular Physics*.**37**(5): 1429–1454. Bibcode:1979MolPh..37.1429N. doi:10.1080/00268977900101051. ISSN 0026-8976.**^**Feng, Chao; Schultz, Andrew J.; Chaudhary, Vipin; Kofke, David A. (2015-07-28). "Eighth to sixteenth virial coefficients of the Lennard-Jones model".*The Journal of Chemical Physics*.**143**(4): 044504. Bibcode:2015JChPh.143d4504F. doi:10.1063/1.4927339. ISSN 0021-9606. PMID 26233142.**^**Schultz, Andrew J.; Kofke, David A. (2009-11-10). "Sixth, seventh and eighth virial coefficients of the Lennard-Jones model".*Molecular Physics*.**107**(21): 2309–2318. Bibcode:2009MolPh.107.2309S. doi:10.1080/00268970903267053. ISSN 0026-8976. S2CID 94811614.**^**Bell, Ian H.; Messerly, Richard; Thol, Monika; Costigliola, Lorenzo; Dyre, Jeppe C. (2019-07-25). "Modified Entropy Scaling of the Transport Properties of the Lennard-Jones Fluid".*The Journal of Physical Chemistry B*.**123**(29): 6345–6363. doi:10.1021/acs.jpcb.9b05808. ISSN 1520-6106. PMC 7147083. PMID 31241958.**^**Lautenschlaeger, Martin P.; Hasse, Hans (2019). "Transport properties of the Lennard-Jones truncated and shifted fluid from non-equilibrium molecular dynamics simulations".*Fluid Phase Equilibria*.**482**: 38–47. doi:10.1016/j.fluid.2018.10.019. S2CID 106113718.- ^
^{a}^{b}^{c}Travesset, Alex (2014-10-28). "Phase diagram of power law and Lennard-Jones systems: Crystal phases".*The Journal of Chemical Physics*.**141**(16): 164501. Bibcode:2014JChPh.141p4501T. doi:10.1063/1.4898371. ISSN 0021-9606. PMID 25362319. **^**Hansen, Jean-Pierre; Verlet, Loup (1969-08-05). "Phase Transitions of the Lennard-Jones System".*Physical Review*.**184**(1): 151–161. Bibcode:1969PhRv..184..151H. doi:10.1103/PhysRev.184.151. ISSN 0031-899X.**^**Longuet-Higgins, H.C. (1951-02-07). "The statistical thermodynamics of multicomponent systems".*Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences*.**205**(1081): 247–269. Bibcode:1951RSPSA.205..247L. doi:10.1098/rspa.1951.0028. ISSN 0080-4630. S2CID 202575459.**^**Leland, T. W.; Rowlinson, J. S.; Sather, G. A. (1968). "Statistical thermodynamics of mixtures of molecules of different sizes".*Transactions of the Faraday Society*.**64**: 1447. doi:10.1039/tf9686401447. ISSN 0014-7672.**^**Mansoori, G. Ali; Leland, Thomas W. (1972). "Statistical thermodynamics of mixtures. A new version for the theory of conformal solution".*Journal of the Chemical Society, Faraday Transactions 2*.**68**: 320. doi:10.1039/f29726800320. ISSN 0300-9238.**^**Rowlinson, J.S.; Swinton, F.L. (1982).*Liquids and liquid mixtures*(Third ed.). London: Butterworth.- ^
^{a}^{b}Deiters, Ulrich K.; Kraska, Thomas (2012).*High-pressure fluid phase equilibria : phenomenology and computation*(1st ed.). Amsterdam: Elsevier. ISBN 978-0-444-56354-5. OCLC 787847134. **^**Schnabel, Thorsten; Vrabec, Jadran; Hasse, Hans (2007). "Unlike Lennard–Jones parameters for vapor–liquid equilibria".*Journal of Molecular Liquids*.**135**(1–3): 170–178. arXiv:0904.4436. doi:10.1016/j.molliq.2006.12.024. S2CID 16111477.**^**Lorentz, H. A. (1881). "Ueber die Anwendung des Satzes vom Virial in der kinetischen Theorie der Gase".*Annalen der Physik*(in German).**248**(1): 127–136. Bibcode:1881AnP...248..127L. doi:10.1002/andp.18812480110.**^**van Konynenburg, P.H.; Scott, R.L. (1980-12-18). "Critical lines and phase equilibria in binary van der Waals mixtures".*Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences*.**298**(1442): 495–540. Bibcode:1980RSPTA.298..495K. doi:10.1098/rsta.1980.0266. ISSN 0080-4614. S2CID 122538015.**^**Potoff, Jeffrey J.; Panagiotopoulos, Athanassios Z. (1998-12-22). "Critical point and phase behavior of the pure fluid and a Lennard-Jones mixture".*The Journal of Chemical Physics*.**109**(24): 10914–10920. Bibcode:1998JChPh.10910914P. doi:10.1063/1.477787. ISSN 0021-9606.**^**Protsenko, Sergey P.; Baidakov, Vladimir G. (2016). "Binary Lennard-Jones mixtures with highly asymmetric interactions of the components. 1. Effect of the energy parameters on phase equilibria and properties of liquid-gas interfaces".*Fluid Phase Equilibria*.**429**: 242–253. doi:10.1016/j.fluid.2016.09.009.**^**Protsenko, Sergey P.; Baidakov, Vladimir G.; Bryukhanov, Vasiliy M. (2016). "Binary Lennard-Jones mixtures with highly asymmetric interactions of the components. 2. Effect of the particle size on phase equilibria and properties of liquid-gas interfaces".*Fluid Phase Equilibria*.**430**: 67–74. doi:10.1016/j.fluid.2016.09.022.**^**Stephan, Simon; Hasse, Hans (2020-01-23). "Molecular interactions at vapor-liquid interfaces: Binary mixtures of simple fluids".*Physical Review E*.**101**(1): 012802. Bibcode:2020PhRvE.101a2802S. doi:10.1103/PhysRevE.101.012802. ISSN 2470-0045. PMID 32069593. S2CID 211192904.- ^
^{a}^{b}Lamm, Monica H.; Hall, Carol K. (2002). "Equilibria between solid, liquid, and vapor phases in binary Lennard–Jones mixtures".*Fluid Phase Equilibria*. 194–197: 197–206. doi:10.1016/S0378-3812(01)00650-1. - ^
^{a}^{b}Lamm, Monica H.; Hall, Carol K. (2001). "Monte Carlo simulations of complete phase diagrams for binary Lennard–Jones mixtures".*Fluid Phase Equilibria*.**182**(1–2): 37–46. doi:10.1016/S0378-3812(01)00378-8. - ^
^{a}^{b}Hitchcock, Monica R.; Hall, Carol K. (1999-06-15). "Solid–liquid phase equilibrium for binary Lennard-Jones mixtures".*The Journal of Chemical Physics*.**110**(23): 11433–11444. Bibcode:1999JChPh.11011433H. doi:10.1063/1.479084. ISSN 0021-9606. **^**Jungblut, Swetlana; Dellago, Christoph (2011-03-14). "Crystallization of a binary Lennard-Jones mixture".*The Journal of Chemical Physics*.**134**(10): 104501. Bibcode:2011JChPh.134j4501J. doi:10.1063/1.3556664. ISSN 0021-9606. PMID 21405169.- ^
^{a}^{b}Lamm, Monica H.; Hall, Carol K. (2004). "Effect of pressure on the complete phase behavior of binary mixtures".*AIChE Journal*.**50**(1): 215–225. doi:10.1002/aic.10020. ISSN 0001-1541. **^**Cotterman, R. L.; Prausnitz, J. M. (1986). "Molecular thermodynamics for fluids at low and high densities. Part II: Phase equilibria for mixtures containing components with large differences in molecular size or potential energy".*AIChE Journal*.**32**(11): 1799–1812. doi:10.1002/aic.690321105. ISSN 0001-1541.**^**Müller, Andreas; Winkelmann, Jochen; Fischer, Johann (1996). "Backone family of equations of state: 1. Nonpolar and polar pure fluids".*AIChE Journal*.**42**(4): 1116–1126. doi:10.1002/aic.690420423. ISSN 0001-1541.**^**Weingerl, Ulrike; Wendland, Martin; Fischer, Johann; Müller, Andreas; Winkelmann, Jochen (2001). "Backone family of equations of state: 2. Nonpolar and polar fluid mixtures".*AIChE Journal*.**47**(3): 705–717. doi:10.1002/aic.690470317.- ^
^{a}^{b}Lafitte, Thomas; Apostolakou, Anastasia; Avendaño, Carlos; Galindo, Amparo; Adjiman, Claire S.; Müller, Erich A.; Jackson, George (2013-10-16). "Accurate statistical associating fluid theory for chain molecules formed from Mie segments".*The Journal of Chemical Physics*.**139**(15): 154504. Bibcode:2013JChPh.139o4504L. doi:10.1063/1.4819786. hdl:10044/1/12859. ISSN 0021-9606. PMID 24160524. **^**Blas, F.J.; Vega, L.F. (1997). "Thermodynamic behaviour of homonuclear and heteronuclear Lennard-Jones chains with association sites from simulation and theory".*Molecular Physics*.**92**(1): 135–150. Bibcode:1997MolPh..92..135F. doi:10.1080/002689797170707. ISSN 0026-8976.**^**Kraska, Thomas; Gubbins, Keith E. (1996). "Phase Equilibria Calculations with a Modified SAFT Equation of State. 1. Pure Alkanes, Alkanols, and Water".*Industrial & Engineering Chemistry Research*.**35**(12): 4727–4737. doi:10.1021/ie9602320. ISSN 0888-5885.**^**Ghonasgi, D.; Chapman, Walter G. (1994). "Prediction of the properties of model polymer solutions and blends".*AIChE Journal*.**40**(5): 878–887. doi:10.1002/aic.690400514. ISSN 0001-1541.**^**Mecke, M.; Müller, A.; Winkelmann, J.; Vrabec, J.; Fischer, J.; Span, R.; Wagner, W. (1996-03-01). "An accurate Van der Waals-type equation of state for the Lennard-Jones fluid".*International Journal of Thermophysics*.**17**(2): 391–404. Bibcode:1996IJT....17..391M. doi:10.1007/BF01443399. ISSN 1572-9567. S2CID 123304062.- ^
^{a}^{b}^{c}^{d}^{e}Kolafa, Jiří; Nezbeda, Ivo (1994). "The Lennard-Jones fluid: an accurate analytic and theoretically-based equation of state".*Fluid Phase Equilibria*.**100**: 1–34. doi:10.1016/0378-3812(94)80001-4. **^**Thol, Monika; Rutkai, Gabor; Köster, Andreas; Lustig, Rolf; Span, Roland; Vrabec, Jadran (2016). "Equation of State for the Lennard-Jones Fluid".*Journal of Physical and Chemical Reference Data*.**45**(2): 023101. Bibcode:2016JPCRD..45b3101T. doi:10.1063/1.4945000. ISSN 0047-2689.**^**Gottschalk, Matthias (2019-12-01). "An EOS for the Lennard-Jones fluid: A virial expansion approach".*AIP Advances*.**9**(12): 125206. Bibcode:2019AIPA....9l5206G. doi:10.1063/1.5119761. ISSN 2158-3226.- ^
^{a}^{b}Johnson, J. Karl; Zollweg, John A.; Gubbins, Keith E. (1993-02-20). "The Lennard-Jones equation of state revisited".*Molecular Physics*.**78**(3): 591–618. Bibcode:1993MolPh..78..591J. doi:10.1080/00268979300100411. ISSN 0026-8976. **^**Vrabec, Jadran; Kedia, Gaurav Kumar; Fuchs, Guido; Hasse, Hans (2006-05-10). "Comprehensive study of the vapour–liquid coexistence of the truncated and shifted Lennard–Jones fluid including planar and spherical interface properties".*Molecular Physics*.**104**(9): 1509–1527. Bibcode:2006MolPh.104.1509V. doi:10.1080/00268970600556774. ISSN 0026-8976. S2CID 96606562.**^**Heier, Michaela; Stephan, Simon; Liu, Jinlu; Chapman, Walter G.; Hasse, Hans; Langenbach, Kai (2018-08-18). "Equation of state for the Lennard-Jones truncated and shifted fluid with a cut-off radius of 2.5 σ based on perturbation theory and its applications to interfacial thermodynamics".*Molecular Physics*.**116**(15–16): 2083–2094. Bibcode:2018MolPh.116.2083H. doi:10.1080/00268976.2018.1447153. ISSN 0026-8976. S2CID 102956189.**^**Shaul, Katherine R. S.; Schultz, Andrew J.; Kofke, David A. (2010). "The effect of truncation and shift on virial coefficients of Lennard–Jones potentials".*Collection of Czechoslovak Chemical Communications*.**75**(4): 447–462. doi:10.1135/cccc2009113. ISSN 1212-6950.**^**Shi, Wei; Johnson, J.Karl (2001). "Histogram reweighting and finite-size scaling study of the Lennard–Jones fluids".*Fluid Phase Equilibria*. 187–188: 171–191. doi:10.1016/S0378-3812(01)00534-9.- ^
^{a}^{b}Dunikov, D. O.; Malyshenko, S. P.; Zhakhovskii, V. V. (2001-10-08). "Corresponding states law and molecular dynamics simulations of the Lennard-Jones fluid".*The Journal of Chemical Physics*.**115**(14): 6623–6631. Bibcode:2001JChPh.115.6623D. doi:10.1063/1.1396674. ISSN 0021-9606. **^**Lívia B. Pártay, Christoph Ortner, Albert P. Bartók, Chris J. Pickard and Gábor Csányi "Polytypism in the ground state structure of the Lennard-Jonesium", Physical Chemistry Chemical Physics**19**19369 (2017)**^**Tchipev, Nikola; Seckler, Steffen; Heinen, Matthias; Vrabec, Jadran; Gratl, Fabio; Horsch, Martin; Bernreuther, Martin; Glass, Colin W; Niethammer, Christoph; Hammer, Nicolay; Krischok, Bernd (2019). "TweTriS: Twenty trillion-atom simulation".*The International Journal of High Performance Computing Applications*.**33**(5): 838–854. doi:10.1177/1094342018819741. ISSN 1094-3420. S2CID 59345875.**^**Stephan, Simon; Liu, Jinlu; Langenbach, Kai; Chapman, Walter G.; Hasse, Hans (2018). "Vapor−Liquid Interface of the Lennard-Jones Truncated and Shifted Fluid: Comparison of Molecular Simulation, Density Gradient Theory, and Density Functional Theory".*The Journal of Physical Chemistry C*.**122**(43): 24705–24715. doi:10.1021/acs.jpcc.8b06332. ISSN 1932-7447. S2CID 105759822.**^**Pedersen, Ulf R.; Schrøder, Thomas B.; Dyre, Jeppe C. (2018-04-20). "Phase Diagram of Kob-Andersen-Type Binary Lennard-Jones Mixtures".*Physical Review Letters*.**120**(16): 165501. arXiv:1803.08956. Bibcode:2018PhRvL.120p5501P. doi:10.1103/PhysRevLett.120.165501. PMID 29756931. S2CID 206310071.**^**Kob, Walter; Andersen, Hans C. (1995-05-01). "Testing mode-coupling theory for a supercooled binary Lennard-Jones mixture I: The van Hove correlation function".*Physical Review E*.**51**(5): 4626–4641. arXiv:cond-mat/9501102. Bibcode:1995PhRvE..51.4626K. doi:10.1103/PhysRevE.51.4626. PMID 9963176. S2CID 17662741.**^**Grüneisen, Edward (1911). "Das Verhältnis der thermischen Ausdehnung zur spezifischen Wärme fester Elemente".*Zeitschrift für Elektrochemie und angewandte physikalische Chemie*.**17**: 737–739. doi:10.1002/bbpc.191100004 (inactive 31 October 2021).CS1 maint: DOI inactive as of October 2021 (link)**^**Grüneisen, E. (1912). "Theorie des festen Zustandes einatomiger Elemente".*Annalen der Physik*(in German).**344**(12): 257–306. Bibcode:1912AnP...344..257G. doi:10.1002/andp.19123441202.**^**Stockmayer, W. H. (1941-05-01). "Second Virial Coefficients of Polar Gases".*The Journal of Chemical Physics*.**9**(5): 398–402. Bibcode:1941JChPh...9..398S. doi:10.1063/1.1750922. ISSN 0021-9606.

- Lennard-Jones model on SklogWiki.