One modification to this equation involves adding an embedded magnetic dipole. Kihara generalized it to account for non-spherical bodies. Barker and Henderson used a temperature-dependent diameter term in a perturbation theory used with this equation. In addition to the Stockmayer modification of it, another method decomposes the model into two piecewise terms, both with a change at two to the 1/6 sigma. A truncated version sets it to zero at 2.5 times sigma, and it is the basis of the Weeks-Chandler-Andersen perturbation theory. This equation has a coefficient equal to four times the well depth. One of its terms is based on the Pauli exclusion principle. For 10 points, name this potential used to model molecules, that has a 6th power attra
One modification to this equation involves adding an embedded magnetic dipole. Kihara generalized it to account for non-spherical bodies. Barker and Henderson used a temperature-dependent diameter term in a perturbation theory used with this equation. In addition to the Stockmayer modification of it, another method decomposes the model into two piecewise terms, both with a change at two to the 1/6 sigma. A truncated version sets it to zero at 2.5 times sigma, and it is the basis of the Weeks-Chandler-Andersen perturbation theory. This equation has a coefficient equal to four times the well depth. One of its terms is based on the Pauli exclusion principle. For 10 points, name this potential used to model molecules, that has a 6th power attractive and 12th power repulsive term.
One modification to this equation involves adding an embedded magnetic dipole.
Lennard-Jones potential