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November 8, 2023 15:35
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excel lambda functions
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// Dispersion force Models | |
// See <https://arxiv.org/pdf/1910.05746.pdf> | |
// In these expressions, the unit of length is /sigma, the interparticle | |
// distance where the potential changes sign and the unit of energy is | |
// /epsilon, the well depth. | |
// | |
/* Lennard-Jones Potential | |
Inputs: | |
rs: separation | |
sigma: interparticle distance where the potential changes sign | |
epsilon: well depth | |
Return: | |
The potential | |
*/ | |
LJ = LAMBDA(rs, sigma_, epsilon_, | |
4 * epsilon_ * ((sigma_ / rs) ^ 12 - (sigma_ / rs) ^ 6) | |
); | |
/* Coefficient that ensures the depth of the attractive well is -epsilon | |
Inputs: | |
rs: separation | |
sigma: interparticle distance where the potential changes sign | |
epsilon: well depth | |
*/ | |
alpha = LAMBDA(rc_, sigma_, | |
2 * (rc_ / sigma_) ^ 2 * | |
(3 / (2 * ((rc_ / sigma_) ^ 2 - 1))) ^ 3 | |
); | |
rmin = LAMBDA(rc_, sigma_, | |
rc_ * (3 / (1 + 2 * (rc_ / sigma_) ^ 2)) ^ 0.5 | |
); | |
/* Alternative to LJ potential | |
Inputs: | |
rs_: separation | |
sigma_: interparticle distance where the potential changes sign | |
epsilon_: well depth | |
rc_: Cut off | |
Return: | |
Modified potential with cutoff at rc_ | |
*/ | |
phi = LAMBDA(rs_, sigma_, epsilon_, rc_, | |
LET( | |
alpha_, alpha(rc_, sigma_), | |
return_, epsilon_ * alpha_ * | |
((sigma_ / rs_) ^ 2 - 1) * | |
((rc_ / rs_) ^ 2 - 1) ^ 2, | |
IF(rs_ <= rc_, return_, 0) | |
) | |
); |
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