Partial charge
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A partial charge is a charge with an absolute value of less than one elementary charge unit (that is, smaller than the charge of the electron).
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[edit] Partial atomic charges
Partial charges are created due to the asymmetric distribution of electrons in chemical bonds. The resulting partial charges are a property only of zones within the distribution, and not the assemblage as a whole. For example, chemists often choose to look at a small space surrounding the nucleus of an atom: When an electrically neutral atom bonds chemically to another neutral atom that is more electronegative, its electrons are partially drawn away. This leaves the region about that atom's nucleus with a partial positive charge, and it creates a partial negative charge on the atom to which it is bonded.
In such a situation, the distributed charges taken as a group always carries a whole number of elementary charge units. Yet one can point to zones within the assemblage where less than a full charge resides, such as the area around an atom's nucleus. This is possible in part because particles are not like mathematical points--which must be either inside a zone or outside it--but are smeared out by the uncertainty principle of quantum mechanics. Because of this smearing effect, if one defines a sufficiently small zone, a fundamental particle may be both partly inside and partly outside it.
[edit] Uses
Partial atomic charges are used in molecular mechanics force fields to compute the electrostatic interaction energy using Coulomb's law. They are also often used for a qualitative understanding of the structure and reactivity of molecules.
[edit] Methods of determining partial atomic charges
Despite its usefulness, the concept of a partial atomic charge is somewhat arbitrary, because it depends on the method used to delimit between one atom and the next (in reality, atoms have no clear boundaries). As a consequence, there are many methods for estimating the partial charges. The following list is taken from Meister and Schwarz, 1994 (see the article for details and references about each method).
- Population analysis of wavefunctions
- Mulliken population analysis
- Coulson's charges
- Natural charges
- CM1, CM2, CM3 charge models
- Partitioning of electron density distributions
- Hirshfeld charges
- Density fitted atomic charges
- Bader charges (obtained from an atoms in molecules analysis)
- Maslen's corrected Bader charges
- Politzer's charges
- Charges derived from density-dependent properties
- Partial derived charges
- Dipole charges
- Dipole derivative charges
- Charges derived from electrostatic potential
- Chelp
- ChelpG, Breneman model
- MK, Merz-Kollman
- Charges derived from spectroscopic data
- Charges from infrared intensities
- Charges from X-ray photoelectron spectroscopy (ESCA)
- Charges from X-ray emission spectroscopy
- Charges from X-ray absorption spectra
- Charges from ligand-field splittings
- Charges from UV-vis intensities of transition metal complexes
- Charges from other spectroscopies, such as NMR, EPR, EQR
- Charges from other experimental data
- Charges from bandgaps or dielectric constants
- Apparent charges from the piezoelectric effect
- Charges derived from adiabatic potential energy curves
- Electronegativity-based charges
- Other physicochemical data, such as equilibrium and reaction rate constants, thermochemistry, and liquid densities.
- Formal charges
[edit] Fundamental particles with non-integer charge
An "up-type quark" has an intrinsic charge of +2/3 of a unit and a "down-type quark" has an intrinsic charge –1/3 of a unit.
[edit] References
J. Meister, W. H. E. Schwarz. Principal Components of Ionicity. J. Phys. Chem. 1994, 98, 8245-8252.

