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Equalizing chaige

This valence bond description leads to an interesting conclusion. Because the transition state occurs at the point where the initial and final state VB configurations cross, the transition state receives equal contributions from each. This is so whether the transition state is early or late. Thus, the nucleophile Y and the leaving group X possess about equal chaige densities in the transition state. This conclusion means that an early transition state is not (in this sense) reactantlike , for a reactantlike transition state should have most of the charge on Y. Similarly, a late transition state is not necessarily productlike. This view is at variance with other interpretations. [Pg.125]

Before discussing structure and bonding in molecules, let s first review some fundfflnen-tals of atomic stmcture. Each element is chaiacterized by a unique atomic number Z, which is equal to the number of protons in its nucleus. A neutral atom has equal numbers of protons, which are positively charged, and electrons, which are negatively chaiged. [Pg.7]

Although Eqs. (14.2) and (14.4) can be solved analytically (as will be shown in the next section), here it is sufficient to use the renowned depletion, or Schott-ky approximation, in which it is assumed that the effective density of chaige is constant and equal to qNd in the depletion region, and zero outside this region. In this case, a double integration of Eq. (14.2) directly gives... [Pg.246]

This equation, known as the Lippmann equation, is perhaps a surprising result The slope of the electrocapillaiy curve at any cell potential Vis equal to the chaige density on the electrode (Fig. 6.55). [Pg.141]

We have seen that electron-transfer reactions can occur at one chaiged plate. What happens if one takes into account the second plate There, the eleetron transfer is from the solution to the plate or electronic conductor. Thus, if we consider the two electronic conductor-ionic conductor interfaces (namely, the whole cell), there is no net electron transfer. The electron outflow from one electronic conductor equals the inflow to the other, that is, a purely chemical reaction (one not involving net electron transfer) can be carried out in an electrochemical cell. Such net reactions in an electrochemical ceU turn out to be formally identical to the familiar thamally induced reactions of ordinary chemistry in which molecules collide with each other and form new species with new bonds. There are, however, fundamental differences between the ordinary chemical way of effecting a reaction and the less familiar electrical or electrochemical way, in which the reactants collide not with each other but with separated charge-transfer catalysts, as the two plates which serve as electron-exchange areas might well be called. One of the differences, of course, pertains to the facility with which the rate of a reaction in an electrochemical cell can be controlled all one has to do is electronically to control the power source. This ease of control arises because the electrochemical reaction rate is the rate at which the power source pushes out and receives back electrons after their journey around the circuit that includes (Figs. 1.4 and lA) the electrochemical cell. [Pg.65]

Electron—A stable elementary particle having an electric charge equal to 1.60210xl0"19 C (Coulombs) and a rest mass equal to 9.1091xl0"31 kg. A positron is a positively chaiged "electron" (see Positron). [Pg.408]

For an accurate measurement using a field voltmeter, the meter must be calibrated (or zeroed) before a test. The chaige on a grounded conductor is measured. A grounded conductor should have a chaige equal to zero, which means the voltage would be zero. Therefore, the field meter should read zero (Fig. 2a). [Pg.289]

When two conducting phases come into contact with each other, a redistribution of chaige occurs as a result of any electron energy level difference between the phases. If the two phases are metals, electrons flow from one metal to the other until the electron levels equilibrate. When an electrode, ie, electronic conductor, is immersed in an electrolyte, ie, ionic conductor, an electrical double layer forms at the electrode—solution interface resulting from the unequal tendency for distribution of electrical charges in the two phases. Because overall electrical neutrality must be maintained, this separation of chaige between the electrode and solution gives rise to a potential difference between the two phases, equal to that needed to ensure equihbrium... [Pg.510]

Fig. IJ.2 Illustration of the reversibility problem. The standard rate constants (1) and s(2)] are characteristic of the chaige transfer rate of the given systems. The diffusion rate constants ( mR or krao) ars varied by the rotation rate of the electrode. If kg g> the system is reversible, while in the case of ks irreversible behavior can be observed. The values of the diffusion coefficients are taken as equal for both systems... Fig. IJ.2 Illustration of the reversibility problem. The standard rate constants (1) and s(2)] are characteristic of the chaige transfer rate of the given systems. The diffusion rate constants ( mR or krao) ars varied by the rotation rate of the electrode. If kg g> the system is reversible, while in the case of ks irreversible behavior can be observed. The values of the diffusion coefficients are taken as equal for both systems...
Dolenko GN, Voronkov MG, EUn VP, Yumatov VD (1993) X-ray investigation of the electron structure of oiganic compounds containing SiS and SiO bonds. J Molec Struct 295 113-120 JoUy WL, Perry WB (1974) Calculation of atomic chaiges by an electronegativity equalization procedure. Inoig Chem 13 2686-2692... [Pg.141]

Uytterhoeven L, Mortier WJ, Geerlings P (1989) Chaige distribution and effective electronegativity of aluminophosphate frameworks. J Phys Chem Solids 50 479-486 De Proft F, Langenaeker W, Geerlings P( 1995) A non-empirical electronegativity equalization scheme theory and applications using isolated atom properties. J Mol Struct Theochem... [Pg.155]

Notice that the shared electron density, P, is divided equally between the two atoms in question. Hie gross atomic chaige on each atom is simply the sum of all the q,i, belonging to that atom minus the nuclear diarge of the atom on which or-bi Xii is located. [Pg.248]

So, for the tetrahedron [SiOJ we have the cation chaige z=4, coordinated to a number of anions equal to n=4, which results in an electrostatic valence of the cation equal to p=4/4=l, while the valenee of the anion is y=2, concluding the equality 1=2/2 p=y/2). [Pg.429]

The mesodosmic structures form every time the number of coordination of the cation equaling to its chaige, which happens when the electrostatic valence of a cation froming a lattice is unity (1). [Pg.429]

Dipole moment (p) The product of the distance separating opposite charges of equal magnitude and the magnitude of the chaige a measure of the polarity of a bond or molecule. A measured dipole moment refers to the dipole moment of an entire molecule. [Pg.280]

In a sense, each atom s oxidation number makes a contribution to the overall charge on the species. Note that the oxidation numbers in both HF [(+1) -h (-1) = 0] and NH3 [(—3) + 3(+1) = 0] sum to zero. Because compounds are electrically neutral, the oxidation numbers in any compound will sum to zero. For a polyatomic ion, oxidation numbers must sum to the chaige on the ion. (The oxidation number of a monatomic ion is equal to its chaige.)... [Pg.130]

Equal-sized spheres (general) and x/ > 10 Two cases Case 1. Constant surface potential (chaige controlled by the concentration of potential-determining ions in solution). Works well for all separations, H. Case 2. Constant surface chaige (e.g. isomorphous substitution in a lattice). Should be used with caution, especially at close approach (Goodwin, 2009). V/R = 2)ueeofVol ( +e Vr = 2)ueeoRv ln(l e... [Pg.230]


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