Charge equilibration for molecular dynamics simulations: Difference between revisions

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:<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>
:<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.
where <math>\phi</math> represents a normalised ''ns'' Slater-type orbital.


==Split-charge formalism==
==Split-charge formalism==
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==See also==
==See also==
*[[Drude oscillators]]
*[[Drude oscillators]]
*[[Polarizable point dipoles]]
==References==
==References==
<references/>
<references/>

Latest revision as of 14:54, 16 December 2010

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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[edit]

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[edit]

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 a normalised ns Slater-type orbital.

Split-charge formalism[edit]

[5]

Fluctuating-charge formalism[edit]

QTPIE[edit]

[6]

See also[edit]

References[edit]