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).
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 you define a sufficiently small zone, a fundamental particle may be both partly inside and partly outside it.
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.
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
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★
Mulliken population analysis
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Coulson's charges
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★ Natural charges
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★ CM1, CM2,
CM3 charge models
★ Partitioning of
electron density distributions
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Hirshfield charges
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★ Density fitted atomic charges
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★ Bader charges (obtained from an
atoms in molecules analysis)
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★ Maslen's corrected Bader charges
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Politzer's charges
★ Charges derived from density-dependent properties
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Partial derived charges
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Dipole charges
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★ Dipole derivative charges
★ Charges derived from
spectroscopic data
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★ Charges from infrared intensities
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★ Charges from
X-ray photoelectron spectroscopy (ESCA)
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★ Charges from
X-ray emission spectroscopy
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★ Charges from
X-ray absorption spectra
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★ Charges from
ligand-field splittings
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★ Charges from
UV-vis intensities of transition metal complexes
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★ Charges from other spectroscopies, such as
NMR,
EPR,
EQR
★ Charges from other experimental data
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★ Charges from
bandgaps or
dielectric constants
★
★ Apparent charges from the
piezoelectric effect
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★ Charges derived from
adiabatic potential energy curves
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Electronegativity-based charges
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★ Other physicochemical data, such as
equilibrium and
reaction rate constants,
thermochemistry, and liquid densities.
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Formal charges
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.
References
J. Meister, W. H. E. Schwarz. Principal Components of Ionicity. ''J. Phys. Chem.'' '1994', ''98'', 8245-8252.