Editing Stockmayer potential
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The '''Stockmayer potential''' consists of the [[Lennard-Jones model]] with an embedded point [[Dipole moment |dipole]]. Thus the Stockmayer potential becomes | The '''Stockmayer potential''' consists of the [[Lennard-Jones model]] with an embedded point [[Dipole moment |dipole]]. Thus the Stockmayer potential becomes: | ||
:<math> \Phi_{12}(r, \theta_1, \theta_2, \phi) = 4 \epsilon \left[ \left(\frac{\sigma}{r} \right)^{12}- \left( \frac{\sigma}{r}\right)^6 \right] - \frac{\mu_1 \mu_2}{4\pi \epsilon_0 r^3} \left(2 \cos \theta_1 \cos \theta_2 - \sin \theta_1 \sin \theta_2 \cos \phi\right) </math> | :<math> \Phi_{12}(r, \theta_1, \theta_2, \phi) = 4 \epsilon \left[ \left(\frac{\sigma}{r} \right)^{12}- \left( \frac{\sigma}{r}\right)^6 \right] - \frac{\mu_1 \mu_2}{4\pi \epsilon_0 r^3} \left(2 \cos \theta_1 \cos \theta_2 - \sin \theta_1 \sin \theta_2 \cos \phi\right) </math> |