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Equilibrium position summary

Of the adjustable parameters in the Eyring viscosity equation, kj is the most important. In Sec. 2.4 we discussed the desirability of having some sort of natural rate compared to which rates of shear could be described as large or small. This natural standard is provided by kj. The parameter kj entered our theory as the factor which described the frequency with which molecules passed from one equilibrium position to another in a flowing liquid. At this point we will find it more convenient to talk in terms of the period of this vibration rather than its frequency. We shall use r to symbolize this period and define it as the reciprocal of kj. In addition, we shall refer to this characteristic period as the relaxation time for the polymer. As its name implies, r measures the time over which the system relieves the applied stress by the relative slippage of the molecules past one another. In summary. [Pg.98]

In summary, it should be kept in mind that a Huang-Rhys parameter of 0.3 must still be regarded as very small. This becomes obvious when this value is compared to the observed range of S values. These are frequently larger than one and one also finds S values greater than ten for other compounds (e.g. compare Refs. [96-101]). Therefore, the results foimd for Pd(2-thpy)2 show that the nuclear equilibrium positions of the triplet state Tj and of the ground state Sq are rather similar. [Pg.96]

We have seen how Le Chatelier s principle can be used to predict the effect of several types of changes on a system at equilibrium. As a summary of these ideas, Table 6.4 shows how various changes affect the equilibrium position of the endothermic reaction... [Pg.216]

As was first shown by Marcus [21], the transition probability is described by relation (12). In case of the strong bond, an essential peculiarity of the nonradiative transitions is their statistical cooperative character determined by participation of many vibrational degrees of freedom in the transition. Due to this the summary strong bond with the medium is provided by the large number of relatively weak interactions with its individual modes for each interaction the equilibrium position shift is comparable to the zero-point vibration amplitude Sf- ... [Pg.356]

SUMMARY OF FACTORS THAT MAY AFFECT THE EQUILIBRIUM POSITION ... [Pg.584]

The Efifect of a Catalyst Summary of Factors That May Affect the Equilibrium Position... [Pg.496]

In a polyatomic molecule there are several bond lengths and bond angles that can oscillate about their equilibrium values. However, each bond length or bond angle does not oscillate independently of the others. It turns out that there are collective motions of some or all of the nuclei that can oscillate independently, called normal modes. Determining the normal modes is a complicated process, and we give only a brief summary. Some software packages such as CAChe and Spartan carry out the process automatically. We assume that the molecule cannot rotate and is in a fixed orientation. For the first nucleus, let <71 be the displacement of the nucleus from its equilibrium position in the x direction, let q2 be its displacement in the y direction, and qs be its displacement in the z direction. For the second nucleus, let q4, qs, and qe be similar displacements, and so on. There are 3n such variables if there are n nuclei. [Pg.937]

Now imagine adding some acid to the solution - either by mistake or deliberately. Clearly, the concentration of H+ will increase. To prevent the value of Ka changing, some of the hydrogen phosphate ions combine with the additional protons to form dihydrogen phosphate (i.e. Equation (6.48) in reverse). The position of the equilibrium adjusts quickly and efficiently to mop up the extra protons in the buffer solution. In summary, the pH is prevented from changing because protons are consumed. [Pg.270]

Summary of Published Work on the Position of Conformational Equilibrium in N-Methylpiperidine... [Pg.61]

In summary, experimental data on the isomeric abundances at anomeric equilibrium reveal that the preference for the axial position depends on several, interconnected factors which were clarified in surveys on carbohydrate stereochemistry, and these provided a background for ensuing theoretical studies. The elucidation of this relationship in complex carbohydrates is greatly facilitated by measurements on the simple derivatives of oxane, and qualitative trends have already been established. Table II illustrates sever possibilities of the quantification of the energetic aspect of the anomeric effect. The procedure most frequently used, based on Eq. 7, suffers from the ambiguity of the A values for the oxane ring and by their presumed variation with solvent. [Pg.69]

PROMETAPHASE. No entirely satisfactory hypothesis of prometaphase congression is available. The chief issues are the extent to which poleward forces are responsible and, of course, the mechanism of force production or regulation which produces a stable chromosome position midway between the poles. Consideration of the force equilibrium hypothesis of Ostergren (summary 1950 see also Rashevsky, 1941 and Ostergren et al., 1960) illustrates the problems. The hypothesis postulates, first, poleward forces at the kinetochores of each chromosome (or bivalent). If these kinetochores are oriented to... [Pg.242]

Summary The conformational equilibrium of the title compound has been investigated experimentally in the gas phase by gas electron diffraction and in solution at low temperatures by NMR, and theoretically by quantum chemical calculations. Both experimental methods result in a preference of the equatorial position of the methyl group, 68(7)% in the gas phase at 298 K and 74(1)% in solution at 110 K. The calculations predict 66 % equatorial conformer at room temperature. [Pg.135]

The reason is as follows in gases the molecules are present in the free state they move for most of the time without being influenced by any forces, so that it is possible to employ statistical methods and to obtain data which, though summary, are sufficient to characterize the macroscopic state. In the crystal, on the other hand, the mutual forces are so strong that the individual particles are maintained permanently in certain positions of equilibrium and execute vibrations about these. It is possible here to connect the structure with the properties in a purely dynamic way. [Pg.177]

Table 7.5 A broad summary of the effects of changing conditions on the position of an equilibrium... [Pg.235]

In summary, AG can be used to predict the spontaneity of a reaction and position of equilibrium as follows ... [Pg.600]

In summary, a temperature increase favors an endothermic reaction, and a temperature decrease favors an exothermic process. Temperature affects the position of an equilibrium by changing the value of the equilibrium constant. Figures 15.10 and 15.11 illustrate the effects of various stresses on systems at equUibrium. [Pg.616]

The summary of reactivity feedbacks resulting from Doppler effect, uniform radial expansion, and various sodium voidings in the equilibrium core and during the startup cycle are given in Table XX-4. This table also includes the reactivity worths of the control rod system, the GEM (gas expansion module), and the USS (ultimate shutdown system). The gas expansion module is a device that introduces negative reactivity through gas expansion under temperature increase. Its position in the core is shown in Fig. XX-7 no additional details are provided. The USS is explained further in this section. [Pg.557]


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See also in sourсe #XX -- [ Pg.222 ]




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