coulombic

The surface and the protein are then attracted by Coulombic forces.

This is counter to the trend expected if coulombic energy were the determining factor.

This dipole causes a coulombic attraction between the two molecules.

The absence of Coulombic collapse is a quantum-mechanical effect.

V is the Coulombic potential energy of the ions at that distance:

It is Coulombic (able to carry a charge), conformational, and flexible.

These molecules are attracted mainly by Coulombic forces (see above section), and can adhere very strongly to the surface.

The exclusion is by quantum numbers, not by coulombic repulsion.

The partial charges shorten and strengthen the bond through favorable coulombic interactions.

The Coulombic repulsion of particles having the same electric charge can break the bonds that hold solids together.

At very small distances between the nuclei the repulsive interaction can be regarded as essentially Coulombic.

This domain attaches to the lipid bilayer through strong coulombic interactions.

The Coulombic forces will deflect an electron or hole approaching the ionized impurity.

There is coulombic repulsion between electrons.

This is in error; the true exchange-correlation potential decays much slower in a Coulombic manner.

The potential energy arising from Coulombic nuclei-nuclei repulsions - also known as the nuclear repulsion energy.

The additional neutrons "dilute" the coulombic repulsion.

It is not an easy experimental task to accelerate nucleii of this atomic number with sufficient energy to overcome their coulombic repulsion.

An example of a repulsive effect is a molecule contorting to minimize the coulombic interactions of atoms that hold like charges.

This is because nuclear forces are comparatively stronger than the Coulombic forces associated with the interactions between electrons and protons, that generate heat in chemistry.

It is mainly used as an approximation for the Anderson impurity model in the limit that the Coulombic repulsion tends to infinity.

These are often referred to as exciton solutions and they formally describe Coulombic binding by oppositely charged electrons and holes.

The distances between dots in both types of cells are exactly the same, producing the same Coulombic interactions between the electrons in each cell.

This effect is due to the increased coulombic attractions between the fluorine atoms and the carbon because the carbon has a positive partial charge of 0.76.

For a Coulombic system one can thus, in principle, read off all information necessary for completely specifying the Hamiltonian directly from examining the density distribution.