What is the LJ cohesive energy expression for a 4-atom square configuration?

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SUMMARY

The discussion focuses on deriving the Lennard-Jones (LJ) cohesive energy expression for a four-atom molecule arranged in a square configuration. The total potential energy is expressed as U_{tot}=2N\epsilon[A_{12}(\frac{σ}{a})^{12}-A_{6}(\frac{σ}{a})^{6}]. The equilibrium nearest-neighbor separation, a, is determined under the assumption that the square shape is maintained. Additionally, it is concluded that transitioning to a simple cubic structure can lower the LJ energy further due to stronger cohesive interactions, despite an increase in the number of atoms per unit cell.

PREREQUISITES
  • Understanding of Lennard-Jones potential and its parameters (σ, ε)
  • Familiarity with potential energy concepts in molecular configurations
  • Knowledge of crystal structures, specifically simple cubic, body-centered cubic (bcc), and hexagonal close-packed (hcp)
  • Basic algebra for manipulating equations and understanding equilibrium conditions
NEXT STEPS
  • Study the derivation of Lennard-Jones potential parameters for different molecular configurations
  • Explore the implications of cohesive energy in various crystal structures
  • Learn about the stability of molecular configurations and their energy landscapes
  • Investigate computational methods for modeling molecular interactions, such as molecular dynamics simulations
USEFUL FOR

This discussion is beneficial for chemistry students, materials scientists, and researchers interested in molecular modeling and the thermodynamic properties of materials.

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Homework Statement



i) Write down an expression for the LJ cohesive energy of a molecule consisting of four atoms lying on the corners of a square of side a.
ii) Deduce the equilibrium value of the nearest-neighbour separation, a, assuming the molecule retains its square shape
iii) What other configuration could the molecule adopt that would lower its LJ energy further?

Relevant equation:

U_{tot}=2N\epsilon[A_{12}(\frac{σ}{a})^{12}-A_{6}(\frac{σ}{a})^{6}]

The Attempt at a Solution



I have done parts i) and ii). It is part iii) that I am stuck on. Because bcc, hcp and fcc all have higher N, number of atoms per unit cell, and higher values of A_{12}, making the cohesive energy higher - this is the case, isn't it? So what other configuration could the molecule adopt?
 
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yes and no. you have to realize that U is a potential energy and therefore negative in nature. you have to do work to remove these molecules from their square setup into something else. in a simple cubic structure ( 2 sets of these squares make a simple cubic of 8 atoms), the cohesive energy between the molecules is stronger, and so the the potential U is more negative at the equilibrium position, making these bonds more stable.so yes N increases, and maybe even A12, A6 increase, but U is inherently negative making the cohesive energies stronger.
 

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