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1-E curve

Type V isotherms of water on carbon display a considerable variety of detail, as may be gathered from the representative examples collected in Fig. 5.14. Hysteresis is invariably present, but in some cases there are well defined loops (Fig. 5.14(b). (t ), (capillary-condensed water. Extreme low-pressure hysteresis, as in Fig. 5.14(c) is very probably due to penetration effects of the kind discussed in Chapter 4. [Pg.266]

This equation has the same form of that obtained for solid diffusion control with D,j replaced by the equivalent concentration-dependent diffusivity = pDpj/[ pn]Ki l - /i,//i)) ]. Numerical results for the case of adsorption on an initially clean particle are given in Fig. 16-18 for different values of A = = 1 - R. The upt e curves become... [Pg.1520]

Another significant characeristic of the E curve is the variance or the second moment which is... [Pg.2085]

Now, let us define the quantities usually listed as the results of a tensile test. The easiest way to do this is to show them on the (r /e curve itself (Fig. 8.1f). They are ... [Pg.84]

To see what is going on physically, it is easier to return to our first condition. At low stress, if we make a little neck, the material in the neck will work-harden and will be able to carry the extra stress it has to stand because of its smaller area load will therefore be continuous, and the material will be stable. At high stress, the rate of workhardening is less as the true stress-true strain curve shows i.e. the slope of the o/e curve is less. Eventually, we reach a point at which, when we make a neck, the workhardening is only just enough to stand the extra stress. This is the point of necking, with... [Pg.116]

Polythene shows a kind of necking that does not lead to fracture. Figure 11.9 shows its (T /e curve. At quite low stress... [Pg.118]

Figure 8-14. E-curve, F-curve, and A-curve for a typicai system with dead space. Figure 8-14. E-curve, F-curve, and A-curve for a typicai system with dead space.
Similarly, for the step response, the output E-curve from a series of N ideal stirred tanks is... [Pg.717]

For a large amount of dispersion or small value of Np, the pulse response is broad, and it passes the measurement point slowly enough for changes to occur in the shape of the tracer curve. This gives a non-symmetrical E-curve. [Pg.735]

Two types of boundary conditions are considered, the closed vessel and the open vessel. The closed vessel (Figure 8-36) is one in which the inlet and outlet streams are completely mixed and dispersion occurs between the terminals. Piston flow prevails in both inlet and outlet piping. For this type of system, the analytic expression for the E-curve is not available. However, van der Laan [22] determined its mean and variance as... [Pg.736]

Figure C-1 Tensile o, - e. Curve for 3M XP251S Fiberglass-Epoxy (Adapted from [C-1])... Figure C-1 Tensile o, - e. Curve for 3M XP251S Fiberglass-Epoxy (Adapted from [C-1])...
Note T7>e curve above represents values recommended by vanous manufacturers. This curve may be used when the manufacturer is not known. Otherwise, the manufacturer should be consuHed for the applicable correction factor. [Pg.373]

FIG. 20 (a) Density profiles p(z) vs z for e = —2 and four average bulk densities (f> as indicated, (b) Surface excess vs density in the bulk for four choices of e. (c) Profiles for the diagonal components of the pressure tensor and of the total pressure for (p = l.O and e = —2. Insert in (c) shows the difference between P, and Px to show that isotropic behavior in the bulk of the film is nicely obtained, (d) Interfacial tension between the polymer film and the repulsive wall vs bulk density for all four choices of e. Curve is only a guide for the eye [18]. [Pg.598]

Fi -1.70. Polarity reversal of the Al-2n couple in 1 C n sbdium chloriUe hi 25 C., Ciirve a, aluminium and zinc electrodes l J mto apart 16 ml of solutioii per square centimetre of clcc-trh( e curve ft aluminium and zinc electrodes 20 mm apart, 10 ml of solution per square centimetre ofelectrot ... [Pg.233]

It is possible on the basis of this model (arrangement O) to explain the constant capacitance region on the negative side of the C vs. E curve (Fig. 20.7), and why the capacitance in this region is independent of the nature of the cations in the solution. The model of the double layer is shown in Fig. 20.12 in which it can be seen that the surface of the electrode and the... [Pg.1182]

Fig. 4.1.3 Absorption spectra of aequorin (A), spent solution of aequorin after Ca2+-triggered luminescence (B), and the chromophore of aequorin (C). Fluorescence emission spectrum of the spent solution of aequorin after Ca2+-triggered bioluminescence, excited at 340 nm (D). Luminescence spectrum of aequorin triggered with Ca2+ (E). Curve C is a differential spectrum between aequorin and the protein residue (Shimomura et al., 1974b) protein concentration 0.5 mg/ml for A and B, 1.0 mg/ml for C. From Shimomura and Johnson, 1976. Fig. 4.1.3 Absorption spectra of aequorin (A), spent solution of aequorin after Ca2+-triggered luminescence (B), and the chromophore of aequorin (C). Fluorescence emission spectrum of the spent solution of aequorin after Ca2+-triggered bioluminescence, excited at 340 nm (D). Luminescence spectrum of aequorin triggered with Ca2+ (E). Curve C is a differential spectrum between aequorin and the protein residue (Shimomura et al., 1974b) protein concentration 0.5 mg/ml for A and B, 1.0 mg/ml for C. From Shimomura and Johnson, 1976.
The EasQ for Hg, as well as for other liquid metals has been obtained using the Lippman electrometer12 (y, E curve method) modified by Gouy, Frumkin, Koening, and others. The principles of the technique and its problems have been extensively described in previous reviews1,10,16 and will not be dealt with further here. [Pg.33]

There have been many attempts to apply the surface tension (y, E curve) method to solid electrodes, and various experimental approaches... [Pg.33]

The dependence of the C,E curves for a solid metal on the method of electrode surface preparation was reported long ago.10 20 67 70 219-225 in addition to the influence of impurities and faradaic processes, variation in the surface roughness was pointed out as a possible reason for the effect.10 67,70 74 219 For the determination of R it was first proposed to compare the values of C of the solid metal (M) with that of Hg, i.e., R = C-M/c-Hg 10,74.219-221 data at ff=0 for the most dilute solution (usually... [Pg.44]

Frumkin was the first to give a qualitative consideration of the electrochemical properties of pc electrodes.10,20 70 He noted that the charge fixed value of the potential E and this may change the form of the capacitance curve near the diffuse-layer capacitance minimum. Important results were obtained in a pioneering paper by Valette and Hamelin.67 They compared experimental capacitance curves for a pc-Ag electrode and its three basic faces. They found that the capacitance of a pc-Ag electrode can be obtained by the superposition of the corresponding Cj, E curves for individual faces exposed at the pc surface, i.e. [Pg.44]

A weighted sum of C,E curves for the faces was found to be similar to the C,E curve for a pc electrode. According to Valette and Hamelin,67 all main Ag faces [(111), (100), and (110)] are exposed on the surface, their fractions 0j on the surface being 0.31, 0.23, and 0.46, respectively. These authors demonstrated that the diffuse-layer capacitance minimum potential E a of a pc-Ag electrode was only slightly less negative (30 mV) than the pzc of the Ag(110) face, i.e., for the face with the more negative value of EamQ. The diffuse-layer capacitance minimum for pc-Ag was wider and less deep than for the Ag faces. [Pg.45]

Mathematical simulation of C, E curves shows that the shape of the diffuse-layer capacitance minimum depends on the difference of Eamo in individual faces and their fractions, as well as on the shape of partial Cj, E curves (Fig. 9). [Pg.45]

Figure 9. Theoretical C,E curves (1, 2, 3) for single-crystal faces and (4) for a model polycrystalline surface calculated by the superposition of the C,E curves at E= const [Eq. (49)] with = 02 = = 1/3 1. (a) Faces with strong hydrophilicity and (b, c) faces with... Figure 9. Theoretical C,E curves (1, 2, 3) for single-crystal faces and (4) for a model polycrystalline surface calculated by the superposition of the C,E curves at E= const [Eq. (49)] with = 02 = = 1/3 1. (a) Faces with strong hydrophilicity and (b, c) faces with...
Parsons-Zobel plots have been constructed for all the systems at a = 0 in the range 0.02 < c < 0.2 M. These plots were linear, with the value of the slope very close to unity. The values of C, obtained by extrapolation of the C-1, C plots to C a = 0 were in good agreement with those calculated from the C,E curves for the 0.1 M NaC104 + DMF system according to the GCSG model.358 The value of Q increases in the sequence of electrodes Hg < Tl(Ga) < In(Ga) < Ga as the hydrophilicity of the electrode surface rises. [Pg.66]

The electrical double layer at a pc-Ag/aqueous solution interface has been discussed by LeiMs et al., Valette and Hamelin, and Beck et al. in many papers.24 63 67146 223 272363-368 Detailed reviews have been given by Hamelin63 and Vorotyntsev74 in this work only a few comments will be added. First, the diffuse-layer minimum in the C,E curve was obtained363... [Pg.67]


See other pages where 1-E curve is mentioned: [Pg.532]    [Pg.2085]    [Pg.82]    [Pg.83]    [Pg.549]    [Pg.71]    [Pg.689]    [Pg.225]    [Pg.606]    [Pg.333]    [Pg.32]    [Pg.36]    [Pg.37]    [Pg.45]    [Pg.49]    [Pg.51]    [Pg.63]    [Pg.63]    [Pg.65]    [Pg.65]    [Pg.66]    [Pg.72]    [Pg.77]    [Pg.78]   
See also in sourсe #XX -- [ Pg.274 ]

See also in sourсe #XX -- [ Pg.49 ]

See also in sourсe #XX -- [ Pg.327 , Pg.328 ]




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