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    • https://phys.libretexts.org/Bookshelves/Thermodynamics_and_Statistical_Mechanics/Book%3A_Thermodynamics_and_Statistical_Mechanics_(Arovas)/07%3A_Mean_Field_Theory_of_Phase_Transitions/7.02%3A_Fluids_Magnets_and_the_Ising_Model
      For the Lennard-Jones system, V\ns\BR\BR=v(\BR\BR)<0 is due to the attractive tail of the potential, hence J\ns\BR\BR is positive, which prefers alignment of the spins \(\sigma\ns_\B...For the Lennard-Jones system, V\ns\BR\BR=v(\BR\BR)<0 is due to the attractive tail of the potential, hence J\ns\BR\BR is positive, which prefers alignment of the spins σ\ns\BR and σ\ns\BR. and E\ns0=18Nz(\ve\ns\ssrAA+\ve\ns\ssrBB+2\ve\ns\ssrAB), where N is the total number of lattice sites and z=8 is the lattice coordination number, which is the number of nearest neighbors of any given site.

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