Born Mayer Huggins¶
What is it?¶
The Born Mayer Huggins potential is
Equation¶

. is the potential energy
. is the seperation distance between pairs of atoms i-j
. and
. are an adjustable parameters
. and
. are the ion charges
def born_mayer_huggins(A = 1,
r_ij = np.linspace(1,10,100),
p_ij = 1,
qi = 1.602E-19,
qj = 1.602E-19 ):
A=1
r_ij = np.asarray(np.linspace(1,10,100))
p_ij = 1
#short range repulsive force
sr_rep = A*np.exp(-(r_ij)/(p_ij))
qi = 1.602E-19
qj = 1.602E-19
coulomb = np.array([])
#coulombic interaction force computed from Ewald sum method
coulomb = (qi*qj)/(4*con.pi*con.epsilon_0*r_ij)
phi = sr_rep+coulomb
return r_ij, phi
Plot¶
Examples of use¶
When simulating glasses it is important to account for the semi-ionic semi covalent nature. The Born-Mayer-Huggins potential can be used to to represent the “essential structural properties” of silicate or borate glasses. Often times a three body term such as the Stillinger, Weber potential or Feuston and Garofalini potential will be added to the Born Mayer Huggins to account for bonds such as O-Si-O or Si-O-Si [1]. If a modified or extended three body term is added the potential can take into account directional covalent bonding of oxygen atoms in oxide glasses [3]. When simulating oxide glasses it is important to account for coordination number and correctly modellling short-range order of the glass.
References¶
[1] Ghalebb, D. (1996). Molecular dynamics simulation of a nuclear waste glass matrix, 37, 232–236.
[2] Delaye, J. ., Louis-Achille, V., & Ghaleb, D. (1997). Modeling oxide glasses with Born–Mayer–Huggins potentials: Effect of composition on structural changes. Journal of Non-Crystalline Solids, 210(2–3), 232–242. http://doi.org/10.1016/S0022-3093(96)00604-7
[3] Chaussedent, S., Teboul, V., & Monteil, A. (2003). Molecular dynamics simulations of rare-earth-doped glasses. Current Opinion in Solid State and Materials Science, 7(2), 111–116. http://doi.org/10.1016/S1359-0286(03)00050-0