Charge equilibration for molecular dynamics simulations: Difference between revisions

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:<math>\eta = \mathrm{IP - EA} \approx  \frac{\partial^2 E}{\partial Q^2} </math>
:<math>\eta = \mathrm{IP - EA} \approx  \frac{\partial^2 E}{\partial Q^2} </math>
==Charge equilibration energy==
==Charge equilibration energy==
Using the above expressions one has the following expression for the total electrostatic energy (<ref name="GoddardIII"> </ref> Eq. 6)
Using the above expressions one has the following second order approximation for the total electrostatic energy (<ref name="GoddardIII"> </ref> Eq. 6)


:<math>E = \sum_i  \left( q_i\chi_i  +  \frac{q_i^2}{2} \eta_i \right) + \sum_{i \neq j} q_i q_j J_{ij}</math>
:<math>E = \sum_i  \left( q_i\chi_i  +  \frac{q_i^2}{2} \eta_i \right) + \sum_{i \neq j} q_i q_j J_{ij}</math>


The last term is a "shielded" [[Coulomb's law | Coulombic interaction]].
The last term is a "shielded" [[Coulomb's law | Coulombic interaction]], where
 
:<math>J_{ij} ({\mathbf{r}}_{ij}) = \left\langle \phi_i \phi_j  \left\vert \frac{1}{| {\mathbf{r}}_{i} - {\mathbf{r}}_{j}  |} \right\vert \phi_i \phi_j \right\rangle</math>
 
where <math>\phi</math> represents Slater-type orbitals.
 
==Split-charge formalism==
==Split-charge formalism==
<ref>[http://dx.doi.org/10.1063/1.2346671 Razvan A. Nistor, Jeliazko G. Polihronov, Martin H. Müser, and Nicholas J. Mosey "A generalization of the charge equilibration method for nonmetallic materials", Journal of Chemical Physics '''125''' 094108 (2006)]</ref>
<ref>[http://dx.doi.org/10.1063/1.2346671 Razvan A. Nistor, Jeliazko G. Polihronov, Martin H. Müser, and Nicholas J. Mosey "A generalization of the charge equilibration method for nonmetallic materials", Journal of Chemical Physics '''125''' 094108 (2006)]</ref>

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Charge equilibration (QEq) for molecular dynamics simulations [1] [2] is a technique for calculating the distribution of charges within a (large) molecule. This distribution can change with time to match changes in the local environment.

Electronegativity and electronic hardness

The atomic electronegativity is given by [3]

where IP is the ionisation potential, and EA is the electron affinity. The electronic hardness is given by [4]

Charge equilibration energy

Using the above expressions one has the following second order approximation for the total electrostatic energy ([2] Eq. 6)

The last term is a "shielded" Coulombic interaction, where

where represents Slater-type orbitals.

Split-charge formalism

[5]

Fluctuating-charge formalism

QTPIE

[6]

See also

References