Additional hyperconjugative interaction energy stabilization is achieved through an increase in the electronic population of the ? * due to the forming CN bond.
42.
Within this group of chromophores there will be a statistical distribution of solvent-chromophore interaction energies, represented in the figure by a Gaussian distribution function.
43.
The total interaction energy is dependent on three forces : electrostatic repulsion of like charges, vanderWaals attraction between particles, and the effects of solvation.
44.
The long-range interaction energy is the sum of interaction energies between the charges of a central unit cell and all the charges of the lattice.
45.
The long-range interaction energy is the sum of interaction energies between the charges of a central unit cell and all the charges of the lattice.
46.
These interaction energies ( equations below ) describe the particle aggregation process and demonstrate why the St�ber process produces particles that are uniform in size.
47.
The interaction energy is attractive where the curve is negative, and the magnitude of the energy represents the cohesive energy between a pair of atoms.
48.
This is both due to the negative spin-orbit interaction energy and to the reduction in energy resulting from deforming the potential to a more realistic one.
49.
Consequently, there is a negative interaction energy between a dislocation and a precipitate that each respectively cause a compressive and a tensile stress or vice versa.
50.
With a similar method and according to Derjaguin approximation, the van der Waals interaction energy between particles with different shapes can be calculated, such as energy between
