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Relation between A , and

This equation assumes a relation between A and AH. Actually, this is not too hard to prove, as we can show in the following. [Pg.369]

In other words, both summation procedures are valid. They describe different physical situations. In the c-summation the size of the dipolar array is much smaller than the size of the capacitor, while in the p-approach both are equal. One can imagine an infinite number of different summation orders corresponding to different relations between A and Aj, leading to results between the p- and c-limits. To solve the problem unambiguously, one must consider a finite dipolar lattice between finite plates, which requires accounting for edge effects and makes the whole problem much more complicated. [Pg.74]

Figure 3.19 Relation between A and the degree of surface oxidation 0olj)Jt i—Qo/Qu) in anodic-going and cathodic-going potential sweeps at 50mVs l. From Angerstein-Kozlowska... Figure 3.19 Relation between A and the degree of surface oxidation 0olj)Jt i—Qo/Qu) in anodic-going and cathodic-going potential sweeps at 50mVs l. From Angerstein-Kozlowska...
It is only reasonable to suggest that the compressibility of a liquid may depend partly on the shape of the molecules, and that we should, therefore, expect only a rough relation between a- and /S, as we go from one liquid to another. We can eliminate this factor by keeping to the same molecules, for instance, by working with solutions of the same... [Pg.16]

Att —> GO, c becomes independent of t but depends on surfaee roughness, for both types of surface. It can be seen from Figures 15 and 16 that the sealing relation between a and L is. [Pg.388]

Figure 4-17 The relation between a and b. The parameters a and b satisfy Tt aexp(a ) erfc(—a) A few simple relations of the... Figure 4-17 The relation between a and b. The parameters a and b satisfy Tt aexp(a ) erfc(—a) A few simple relations of the...
Dr Price also examined relations between (A) and deton velocity (D). They are presented in Fig 3 for group 1 and in Fig 4 for group 2 Fig 3 shows a representative of group 1, an unconfined cylindrical charge of HBX-1 (RDX/TNT/A1/Wax - 40/38/17/5). Its voidless density is 1.76 g/cc. The curves are for charge diameters d, d, d d which are 6.4, 12.7, 25.4 50.8 mm, respectively. Solid lines are smoothed values from the experimental data which have been extrapolated to A=0.6. The limit line for failure was estimated, as shown on p 694 of Ref 17. A pattern of the same type was previously obtd by Stesik Akimova (Ref 3) for TNT... [Pg.191]

Develop the equivalent of Equation (47) for the surface charge density of a spherical particle (i.e., the relation between a and (d j//dr) evaluated at the surface). [Pg.531]

In most cases of reactions showing a C.E. the relation between A and AE can be represented by the empirical formula... [Pg.77]

As described in Section 1,1, both the procedures of changing Po. at fixed temperature and changing temperature at fixed Po. control the nonstoichiometry in Nii O, Let us consider the relation between a and 3 in Nil O, in which the non-stoichiometry S is believed to originate from metal vacancies. By use of the notation based on the effective charge, described in Section 1,3,7, the chemical equilibrium between the oxygen gas in the atmosphere and the oxygen in the solid may be expressed as... [Pg.60]

There is, moreover, a reasonable relation between a and / . The first quantity is the energy of interchange of two pM electrons, analogous to that of the hydrogen molecule, and the second is the energy of resonance of one electron between two p, orbitals, analogous to that of the... [Pg.204]

Exercise. Apply detailed balance to (3.12) and find a relation between a and jS. Show that they are equal when = V2 and conclude thermodynamics precludes the existence of one-way apertures, or one-way mirrors. [Pg.142]

Derive this, find the equilibrium distribution and the relation between a and / . [Pg.165]

The form of distribution (17) recalls a Boltzmann expression with modulus of distribution 7. Attempts at a direct physical explanation of this result are thwarted by the obvious dependence of 7, not only on the state of the surface, but also on the nature of the gas whose adsorption proceeds according to equation (1). Nevertheless, formula (17) makes very plausible the experimentally observed constancy of the functional dependence A(Q) itself which leads to equation (1). It seems natural that with training or sintering of the surface, the liberation or destruction of points with different heats of adsorption may proceed in such a way as to preserve the exponential relation between A and Q, changing only the constants D, Q0, and especially 7. [Pg.63]

The Formula (55) allows us to evaluate the hydrogen atoms distribution over O and 0 interstitial sites that are determined by temperature, the relation between a and P energy parameters and the total concentration of hydrogen atoms. Based on the relations (55), in the range 0 < c < 3 the dependences for hydrogen atoms distribution in O and interstitial sites are shown in the Figure 17. [Pg.298]

Let us suppose that the field behaves like a cosmological constant for some amount of time. In this case, Eq.(7.24) tells us that the expansion is almost exponential (H Const, a oc eHt). Moreover, the relation between a and r/ is... [Pg.110]

From this, we obtain the relation between a and Mmax... [Pg.117]

Df varying between 2, for a porous electrode, and 3 for a smooth electrode. In the case of a blocked interface, the conclusions up to now are that there is no simple relation between a and the fractal dimension. However, the analogy seems useful from an interpretative point of view. Reviews of the response at fractal and rough electrodes have recently appeared31 32. [Pg.248]

Figure 6 Temperature dependence of the (new) cell parameter a defined in the text for TEA(TCNQ)2. (These data are recalculated from those of Ref. 22 and the unpublished results of A. Filhol and H. Grassi.) Inset Geometrical relation between a and the cell parameters a and b chosen in Ref. 22. Figure 6 Temperature dependence of the (new) cell parameter a defined in the text for TEA(TCNQ)2. (These data are recalculated from those of Ref. 22 and the unpublished results of A. Filhol and H. Grassi.) Inset Geometrical relation between a and the cell parameters a and b chosen in Ref. 22.
The relation between a and the dimensionless heat release a used in Section 2.2.2 is... [Pg.142]

The thermodynamic equations of section 2 are expressed in terms of N, whereas Pn — Pi given in section 3 involves a. We need a relation between a and N. The geometry of a spherical micelle is illustrated in fig. 1 and if v denotes the volume of the hydrocarbon tail of an amphiphile we have the relations... [Pg.248]

Thermal FFF was the first experimentally implemented method [9]. It is used mostly for the fractionation of macromolecules. The temperature difference between two metallic bars, forming the channel walls with highly polished surfaces and separated by a spacer in which the channel proper is cut, produces the flux of the sample components, usually toward the cold wall. The channel for thermal FFF is shown in Fig. 2b. The relation between A and the operational variables is given by... [Pg.678]

Mesopore widths at the maxima of PSDs obtained by the HK method using different relations between A and w. [Pg.232]

Finally we shall derive the relation between a, ], and ar,v The identity... [Pg.59]

Here (5) is an internal relation between A and B, whereas (4) would be an external relation according to the tentative definition. Yet any attempt to define what it means to have power must involve a reference to other people. In one simple conceptualization of power, my amount of allround power is defined as the number of people over tidumt I have control, so that the relational character of power appears explicitly. In another, more complex characterization my power depends on my contrd over resources in which other people have an interest - also a relationally defined property. Similarly, the possession of money must also, if spelled out, involve a reference to other people who are prepared to accept my money as payment for goods. Wittgenstein remarks somewhere that it is impossible to make sense of the statement "It is five o clock on the sun", and it would also be nonsensical to say that Robinson Crusoe on his island could be rich by the mere possession of gold coins. [Pg.94]


See other pages where Relation between A , and is mentioned: [Pg.392]    [Pg.88]    [Pg.121]    [Pg.103]    [Pg.82]    [Pg.457]    [Pg.175]    [Pg.229]    [Pg.386]    [Pg.385]    [Pg.646]    [Pg.284]    [Pg.40]    [Pg.63]    [Pg.76]    [Pg.81]    [Pg.111]    [Pg.112]    [Pg.44]    [Pg.181]    [Pg.169]    [Pg.589]    [Pg.311]    [Pg.15]    [Pg.230]    [Pg.407]   
See also in sourсe #XX -- [ Pg.68 , Pg.69 ]




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