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R curve

The characteristic isotherm concept was elaborated by de Boer and coworkers [90]. By accepting a reference from a BET fit to a standard system and assuming a density for the adsorbed film, one may convert n/rim to film thickness t. The characteristic isotherm for a given adsorbate may then be plotted as t versus P/P. For any new system, one reads t from the standard r-curve and n from the new isotherm, for various P/P values. De Boer and co-work-ers t values are given in Table XVII-4. A plot of t versus n should be linear if the experimental isotherm has the same shape as the reference characteristic isotherm, and the slope gives E ... [Pg.633]

A factor militating against the use of other adsorptives for pore size determination at the present time is the lack of reliable r-curves. The number of published isotherms of vapours such as benzene, carbon tetrachloride or the lower alkanes, or even such simple inorganic substances as carbon dioxide, on a reasonable number of well-defined non-porous adsorbents, is very small. [Pg.167]

ASTM E1152-87, "Determining J—R Curves," A.nnualBook ofJlSTM Standards, ASTM Puhhcations, Philadelphia, 1993. [Pg.550]

Curve with short time rating, but output not exceeding C.M.R. - Curve with short time rating, but output more than C.M.R. [Pg.57]

Having established the various types of bonds that can form between atoms, and the shapes of their potential energy curves, we are now in a position to explore the forces between atoms. Starting with the L/(r) curve, we can find this force F for any separation of the atoms, r, from the relationship... [Pg.43]

Sq can be calculated from the theoretically derived U(r) curves of the sort described in Chapter 4. This is the realm of the solid-state physicist and quantum chemist, but we shall consider one example the ionic bond, for which U(r) is given in eqn. (4.3). Differentiating once with respect to r gives the force between the atoms, which must, of course, be zero at r = rg (because the material would not otherwise be in equilibrium, but would move). This gives the value of the constant B in equation (4.3) ... [Pg.59]

This value can be considerably smaller. It corresponds in Fig. 6-1 to the ordinate of the intersection of the resistance graph of slope cCq with a 7(f/-r) curve that deviates markedly to the left of that plotted. The maximum current density is an important quantity for the setting up of cathodic protection with galvanic anodes and is dependent on the anode geometry and conductivity of the medium. [Pg.185]

Fig. 20-11 Potential-time curves of an enamelled container with built-in stainless steel heat exchanger as a function of equalizing resistance, R. Curve 1 container potential in the region of the heat exchanger. Curve 2 heat exchanger potential in the voltage cone of defects in the enamelling. Curve 3 heat exchanger potential outside the voltage cone of the defects. Fig. 20-11 Potential-time curves of an enamelled container with built-in stainless steel heat exchanger as a function of equalizing resistance, R. Curve 1 container potential in the region of the heat exchanger. Curve 2 heat exchanger potential in the voltage cone of defects in the enamelling. Curve 3 heat exchanger potential outside the voltage cone of the defects.
Specimen size effects have been attributed to rising R-curve behavior for most graphites studied. [Pg.496]

Rising R-curve behavior has been attributed to grain bridging traetions and microcrack dilatation in the eraek wake region. [Pg.496]

To determine the nondimensional side-on impulse 7, read 7 from Figure 6.23 or 6.24 for the appropriate R. Use the curve labeled vessel burst. Fori in the range of 0.1 to 1.0, the 7 versus R curve of Figure 6.24 is more convenient. [Pg.209]

Correction fectors should seldom be used when they fall below a value that lies on a curved portion of the P-R curves. Figure 10-34. That is, values on the straight portions of the curves have litde or no accuracy in most cases. For the single-shell pass—two or more than two passes unit chart, an F of less than about 0.8 would indicate consideration of a two-shell pass unit. As a general guide, F factors less than 0.75 are not used. To raise the F factor, the unit flow system, temperature levels, or both must be changed. [Pg.75]

A typical set of logs recorded while drilling is shown in Figure 4-280. The wireline caliper is shown in the gamma ray track. Displayed on this attachment are gamma ray, R curve, Pe curve, neutron and density curve. The delta-rho curve is the quality curve check for the density log. [Pg.979]

Heyer, R. H., Fracture toughness evaluation by R-curve methods. ASTM, STP 527... [Pg.1358]

Then since R(p) decreases with p, E(p) must increase with p and the E,R curve must be convex downward. Also, from lemma 4-1, E(0) = 0, R(p) 0, and... [Pg.224]

The upper envelope of E as a function of R maximized over p and p can now be found. We first maximize E over p for each value of p numerical techniques or Eqs. (4-104) and (4-106) can be used. Then we maximize this result over p either by using graphical techniques to find the upper envelope or by using Eqs. (4-97) and (4-98). This optimum E,R curve is generally called the reliability curve for the given channel. [Pg.226]

Notice that those distribution functions that satisfy Eq. (4-179) still constitute a convex set, so that optimization of the E,R curve is still straightforward by numerical methods. It is to be observed that the choice of an F(x) satisfying a constraint such as Eq. (4-179) defines an ensemble of codes the individual codes in the ensemble will not necessarily satisfy the constraint. This is unimportant practically since each digit of each code word is chosen independently over the ensemble thus it is most unlikely that the average power of a code will differ drastically from the average power of the ensemble. It is possible to combine the central limit theorem and the techniques used in the last two paragraphs of Section 4.7 to show that a code exists for which each code word satisfies... [Pg.242]

Quantum tunnelling in chemical reactions can be visualised in terms of a reaction coordinate diagram (Figure 2.4). As we have seen, classical transitions are achieved by thermal activation - nuclear (i.e. atomic position) displacement along the R curve distorts the geometry so that the... [Pg.28]

Figure 2.4. Reaction coordinate diagram for a simple chemical reaction. The reactant A is converted to product B. The R curve represents the potential energy surface of the reactant and the P curve the potential energy surface of the product. Thermal activation leads to an over-the-barrier process at transition state X. The vibrational states have been shown for the reactant A. As temperature increases, the higher energy vibrational states are occupied leading to increased penetration of the P curve below the classical transition state, and therefore increased tunnelling probability. Figure 2.4. Reaction coordinate diagram for a simple chemical reaction. The reactant A is converted to product B. The R curve represents the potential energy surface of the reactant and the P curve the potential energy surface of the product. Thermal activation leads to an over-the-barrier process at transition state X. The vibrational states have been shown for the reactant A. As temperature increases, the higher energy vibrational states are occupied leading to increased penetration of the P curve below the classical transition state, and therefore increased tunnelling probability.
While Figure 23.47 shows typical R-curves, all cases will differ to some extent, depending on the site utility configuration, equipment specifications, site heating demand and the parameters assumed to be fixed and those varied in the analysis. [Pg.498]

Figure 12.7. Action spectra for killing (is. coli SD-4 curve I) and for photoreactivation (is. coli B/r, curve II S. griseus, curve III). (Reproduced with permission from Ref. 64.)... Figure 12.7. Action spectra for killing (is. coli SD-4 curve I) and for photoreactivation (is. coli B/r, curve II S. griseus, curve III). (Reproduced with permission from Ref. 64.)...
Emphasis should here be placed on the observations of Holm and Clark (34), according to whom the reaction rate go passes through a maximum when the concentration of a donor impurity is monotonically increased. This maximum may be due, as shown in Fig. 8a, to the transition from the acceptor to the donor branch of the go = go ( [Pg.186]

Fig. 4. Some solutions of the equation (61) for the time development of the dimensionless monatomic density c for the case of irreversible trapping into H2 molecules. Curves show the dependence of c on dimensionless depth f for various values of the dimensionless time r. Curves (a), c(0) = 0.75 curves (b), c(0) = 5.0. Fig. 4. Some solutions of the equation (61) for the time development of the dimensionless monatomic density c for the case of irreversible trapping into H2 molecules. Curves show the dependence of c on dimensionless depth f for various values of the dimensionless time r. Curves (a), c(0) = 0.75 curves (b), c(0) = 5.0.

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