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Residual electrostatic interactions

Thus, the numerical procedure involving the treatment of both the first- and the second-order correlation energies in a complete finite basis demonstrates its high accuracy and flexibility in MBPT calculations. The MBPT version, described in Chapters 3 and 29, provides very accurate results, at least in the range of Z = 10—26. Accounting for the correlation energy due to the residual electrostatic interaction in the second-order of... [Pg.365]

The second hydrophilic slab extends up to 8 nm and contains a much lower segment density (0.1 to 1 per lipid). It is not observed for low-molecu-lar-weight PSS (Mw 4300 Da) and is hardly observed for low salt. Its thickness decreases on film compression toward 2 nm. Qualitatively this thickness decrease can be understood in terms of residual electrostatic interactions between the surface and the polyelectrolyte tails—on compression surface overcharging is reduced and hence the lowered repulsion (from head+PSS in the first slab) enables condensation of the remaining segments in the adjacent slab. [Pg.161]

The combination of and G i with G gives the total energy of interaction, Gp (assuming that there is no contribution from any residual electrostatic interaction), that is [6] ... [Pg.119]

Corrections to the central-field approximation. Two important terms are omitted in the central-field approximation. The first is the residual electrostatic interactions represented by JC (equation (3.68)). This gives rise to non-central forces which cause the motion of the electrons to be correlated with one another, rather than completely independent as in the central-field approximation. The second terra is the magnetic spin-orbit interaction which was not included in equation (3.65) ... [Pg.81]

These selection rules are based on the assumption that L is a good quantum number and that Russell-Saunders coupling is an exact description of the atomic system. This is a good approximation in light atoms where the magnetic interactions are generally very much smaller than the residual electrostatic interactions. However, we may observe transitions which violate equations (5.31) in the spectra of heavier elements. [Pg.134]

By using an effective, distance-dependent dielectric constant, the ability of bulk water to reduce electrostatic interactions can be mimicked without the presence of explicit solvent molecules. One disadvantage of aU vacuum simulations, corrected for shielding effects or not, is the fact that they cannot account for the ability of water molecules to form hydrogen bonds with charged and polar surface residues of a protein. As a result, adjacent polar side chains interact with each other and not with the solvent, thus introducing additional errors. [Pg.364]

How should a molecule be divided into groups In some cases there may appecir to be a chemically obvious way to define the groups, especially when the molecule is a polymer that is constructed from distinct chemical residues. A particularly desirable feature is that each group should, if possible, be of zero charge. The reason for this can be understood if we recall how the different electrostatic interactions vary with distance from Section 4.9.1 ... [Pg.343]

Fig. 6.16 the use of a marker atom on the alpha-carbon in an arginine residue may lead to a significant electrostatic interaction being neglected because the distance between the marker atoms exceeds the cutoff. [Pg.343]

FIGURE 6.1 All electrostatic interaction between the e-amino group of a lysine and the 7-carboxyl group of a glutamate residue. [Pg.160]

Morishima et al. [75, 76] have shown a remarkable effect of the polyelectrolyte surface potential on photoinduced ET in the laser photolysis of APh-x (8) and QPh-x (12) with viologens as electron acceptors. Decay profiles for the SPV (14) radical anion (SPV- ) generated by the photoinduced ET following a 347.1-nm laser excitation were monitored at 602 nm (Fig. 13) [75], For APh-9, the SPV- transient absorption persisted for several hundred microseconds after the laser pulse. The second-order rate constant (kb) for the back ET from SPV- to the oxidized Phen residue (Phen+) was estimated to be 8.7 x 107 M 1 s-1 for the APh-9-SPV system. For the monomer model system (AM(15)-SPV), on the other hand, kb was 2.8 x 109 M-1 s-1. This marked retardation of the back ET in the APh-9-SPV system is attributed to the electrostatic repulsion of SPV- by the electric field on the molecular surface of APh-9. The addition of NaCl decreases the electrostatic interaction. In fact, it increased the back ET rate. For example, at NaCl concentrations of 0.025 and 0.2 M, the value of kb increased to 2.5 x 108 and... [Pg.77]


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Interaction electrostatic

Residual interaction

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