While the properties of essentially localized charge distributions and essentially resonance-delocalized distributions are well understood in chemistry, the changeover region is unique and interesting.
32.
In both cases, we assume that the charge distributions are localized, so that the potentials can be chosen to go to zero at infinity.
33.
They appear naturally in the study of electrostatics in the context of the electrostatic potential associated to a charge distribution on a closed surface.
34.
If both sides of this equation are divided by the volume of this small piece of the charge distribution " dV ", the result is:
35.
Some electrically neutral particles ( like the neutron ) with non-zero spin also have magnetic moment due to the charge distribution in their inner structure.
36.
The electrostatic potential map ( the property of electrostatic potential mapped upon the electron density ) provides an indicator for charge distribution in a molecule.
37.
Problems arise because changes in charge distributions require a non-zero amount of time to be " felt " elsewhere ( required by special relativity ).
38.
The resulting carbanion is stabilized by the structure of the carbanion itself via resonance charge distribution and by the presence of a charged ion prosthetic group.
39.
Packaging of DNA is facilitated by the electrostatic charge distribution : phosphate groups cause DNA to have a negative charge, whilst the histones are positively charged.
40.
In addition, studies have shown that the charge distributions about the active sites are arranged so as to stabilize the transition states of the catalyzed reactions.
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