The coexistence pressures of liquids modeled by this form exhibit a so- called soft sphere asymptote, but are discontinuous at low temperatures, a problem that can be fixed by leveling this function off after its minimum. This function can be modified to account for dipole-dipole interactions through the addition of an anisotropic coefficient over distance cubed. The aforementioned modifications were respectively developed by (*) Weeks, Chandler and Andersen and Stockmayer to extend the applicability of this potential. This potential contains parameters called the well depth and effective diam
The coexistence pressures of liquids modeled by this form exhibit a so- called soft sphere asymptote, but are discontinuous at low temperatures, a problem that can be fixed by leveling this function off after its minimum. This function can be modified to account for dipole-dipole interactions through the addition of an anisotropic coefficient over distance cubed. The aforementioned modifications were respectively developed by (*) Weeks, Chandler and Andersen and Stockmayer to extend the applicability of this potential. This potential contains parameters called the well depth and effective diameter. It respectively models long-range van der Waals attractions and short-range Pauli forces using its distance to the minus six and distance to the minus twelve terms. For 10 points, name this mathematical model of the interaction energy between a pair of neutral molecules, a model named after just one physicist with a compound last name.
The coexistence pressures of liquids modeled by this form exhibit a so- called soft sphere asymptote, but are discontinuous at low temperatures, a problem that can be fixed by leveling this function off after its minimum.
the {Lennard-Jones} potential [prompt on {L-J} potential or {6-12} potential or {12-6} potential]