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Charging normal

Negative formal charges normally reside on the atoms having higher electronegativity. [Pg.107]

Equation (7) guarantees that the minimum in the electrostatic potential is attained at the critical point r defining a sphere 5(0, r ), which contains an electron density amount equal to the atomic number Z. From eq (7) we may conclude that the charge normalization condition for neutral atoms may only be satisfied for r —> oo, whereas for cations it is never satisfied. [Pg.84]

From eq (7) it may be concluded that the charge normalization condition is never satisfied for cations. As a result, the functional dependence of (r) with the radial variable is quite different in this case. For instance, it may be easily shown that 0(r) displays a monotonic decreasing behavior without extrema points along the complete domain of the r variable. As a result, expression (8) for O(r) is not longer valid for singly positive charged atomic systems. [Pg.85]

For anions, the charge normalization condition given in Eq (7) guaran-... [Pg.89]

Figure 8. At r = 0.75, pressure as a function of gi = gis /3 and /re for the normal and color superconducting quark phases (the same as in Figure 7, but from a different viewpoint). The dark solid line represents the mixed phase of negatively charged normal quark matter and positively charged 2SC matter. Figure 8. At r = 0.75, pressure as a function of gi = gis /3 and /re for the normal and color superconducting quark phases (the same as in Figure 7, but from a different viewpoint). The dark solid line represents the mixed phase of negatively charged normal quark matter and positively charged 2SC matter.
Under global charge neutrality condition, assuming that the effect of Coulomb forces and the surface tension is small, one can construct a mixed phase composed of positive charged 2SC phase and negative charged normal quark matter. [Pg.238]

Fig. 7.3 Template model for CYP2D6 with Y the site of oxidation, a is the distance from Y to a heteroatom which is positively charged (normally 5-7 A). Fig. 7.3 Template model for CYP2D6 with Y the site of oxidation, a is the distance from Y to a heteroatom which is positively charged (normally 5-7 A).
The idea is simple. Since SCF Mulliken charges satisfy Eqs. (5.1) and (5.2), we reverse the argument and deduce an internally consistent set of charges starting off with (5.1) and (5.2) and the a constants of Table 5.1. Charge normalization... [Pg.55]

The corresponding correction for hydrogen is as follows, from obvious charge normalization considerations ... [Pg.60]

Another simplification facilitates things because it saves tedious work to satisfy charge normalization constraints. We write Eq. (10.37) as follows... [Pg.125]

See = 69.633 and 8ch = 106.806 kcal/mol. Charge normalization terms are inadvertently treated as part of bond energy Both 8 and 8 are metaphors, not physical entities. In the final count. A, which is usually interpreted as being due to steric effects, is simply a function of local charge variations. [Pg.131]

A drastic approximation had to be made for the hydrogens their total charge was deduced from charge normalization and was entirely treated as atomic charges of hydrogens attached to carbon, i.e. as if was always null in the OH part, which is wrong, of course. [Pg.201]

Direct estimates using the appropriate SCE potentials at the nuclei suggest 181 kcal/mol [141]. The CC and CH parameters are treated the usual way. A general formula is developed as follows. The hydrogen charge variations are expressed relative to q = —W.l me. Charge normalization, (X) c +... [Pg.201]

Any bond energy formula can be expressed either i) by reference to a selected bond with reference net atomic charges q and q°i at the bond-forming atoms k and I, or ii) by reference to hypothetical k-l bonds constructed with the assumption q = q° = 0. The former reflects a physical situation, but requires additional work in order to sadly charge normalization constraints it is most useful in the constmction of general energy formulas for molecules that use chemical shifts espressed with respect to the appropriate references. The latter method simplifies bond-by-bond calculations. The two forms are... [Pg.213]

Fig. 1. (a) The dipole-dipole attraction, illustrated by two molecules of chloromethane favourably orientated, end-to-end in van der Waals contact (b) the dipole-induced-dipole attraction, due to polarization of the right-hand molecule when it comes close to the left-hand molecule. (S signifies a fractional net charge, normally less than the full electronic unit.)... [Pg.10]

Normalization calculations can be tedious, so membrane manufacturers have made available, at no charge, normalization software for their specific membranes. Some chemical vendors and other membrane consultants have software as well, which may or may not be available for public use. Some even have hardware that will download the appropriate data from the PLC or discrete probes to eliminate the need for manual entry of the data. Operators will be able to use the normalization software to review the normalized data, schedule cleanings, and optimize the RO operation. [Pg.247]

Fig. 4. Charge maps of the tetraazacopper(II) complexes. Numerical values near circles and element symbols represent atomic- and bond-charge values, respectively. Circles give the ratio of the atomic-charge (normalized at 40 for a copper atom and 10 for other atom). Fig. 4. Charge maps of the tetraazacopper(II) complexes. Numerical values near circles and element symbols represent atomic- and bond-charge values, respectively. Circles give the ratio of the atomic-charge (normalized at 40 for a copper atom and 10 for other atom).
The electrolyte salt will be consumed stoichiometrically upon charge. Normally A forms the positive and D the negative electrode. For mounting the electrodes in the battery cell, the undoped host lattices are used in conjuction with the concentrated electrolyte. As an alternative, the doped materials are employed, together with the diluted electrolyte. In this case, cycling starts in the discharge direction. [Pg.375]


See other pages where Charging normal is mentioned: [Pg.346]    [Pg.37]    [Pg.42]    [Pg.96]    [Pg.299]    [Pg.13]    [Pg.122]    [Pg.82]    [Pg.76]    [Pg.69]    [Pg.3]    [Pg.4]    [Pg.178]    [Pg.193]    [Pg.194]    [Pg.321]    [Pg.548]    [Pg.29]    [Pg.98]    [Pg.292]    [Pg.62]    [Pg.119]    [Pg.96]    [Pg.32]    [Pg.24]    [Pg.221]    [Pg.1079]    [Pg.206]    [Pg.34]    [Pg.1558]    [Pg.311]    [Pg.568]    [Pg.3]   
See also in sourсe #XX -- [ Pg.29 , Pg.30 ]




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Central normally neutral charge

Normal charge

Normal charge

Normal component of the electric field caused by a planar charge distribution

Normalized integral charge density

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