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S-d model

Finally, we also evaluate the pressure-dependent S-D model in the context of eq. (7.53), which gives the threshold shear resistance in tension where a, as the mean normal stress, is, among other things, also the stress acting across any other plane, thus (7m = <7n- Then, since the first term in eq. (7.53) is the critical shear stress in shear, and the friction coefficient / = (7t/4)y6o = 0.20, we have... [Pg.216]

Selvasekarapandian S., VijayakumarM., Gnanasekaran T., Fujihara S., Koji S. Ion Dynamic Stndies on LaFs Thin Films. Physica B 2003 337 52-57 Shaw-Klein L.J., Bums S.J., Jacobs S.D. Model for laser damage dependence on thin-film morphology. Appl. Opt. 1993 32 3925-3929... [Pg.224]

Using eqs. (37) and (38) and the models proposed by Lang and Ehrenreich (1968), Kanamori (1963), Heine (1967), the equation for the pressure derivative of the Curie temperature in the s-d model was derived (Inoue and Shimizu 1980)... [Pg.108]

Leontiev et al. (1988) used the s-d model to explain the observed nonmonotonic dependence of d In Tq/A In F on the composition in the Dy(Coi tAl t)2 and Tb(Coi j AL)2 compounds. It was shown that the observed maximum could be related to the Fermi level passing through a local maximum on the density of state curve N ) when cobalt was substituted by aluminum. [Pg.110]

Wang L S, Nicholas J B, Dupuis M, Wu FI and Colson S D 1997 SijO (x = 1-6) models for oxidation of silicon surfaces and defect sites in bulk oxide materials Phys. Rev. Lett. 78 4450... [Pg.2407]

In the theory of the liquid state, the hard-sphere model plays an important role. For hard spheres, the pair interaction potential V r) = qo for r < J, where d is the particle diameter, whereas V(r) = 0 for r s d. The stmcture of a simple fluid, such as argon, is very similar to that of a hard-sphere fluid. Hard-sphere atoms do, of course, not exist. Certain model colloids, however, come very close to hard-sphere behaviour. These systems have been studied in much detail and some results will be quoted below. [Pg.2668]

C. N. Montreiul, S. D. WiUiams, and A. A. Adanc2yk, Modeling Current Generation Catalytic Converters Eaboratoy Experiments and Kinetic Parameter Optimisation—Steady State Kinetics, SAE 920096, Society of Automotive Engineers, Warrendale, Pa., 1992. [Pg.496]

Daviskas, E., Gonda, I., and Anderson, S. D. (1990). Mathematical modeling of heat and water transport in human respiratory tract. /. Appl. Physiol. 69, 362-372. [Pg.229]

Peng, S. H. Modeling of turbulent flow and heat transfer for building ventilation. Ph.D. thesis, Dept, of Thermo and Fluid Dynamics, Chalmers University of Technology, Gothenburg, 1998. [Pg.1058]

D. j. Nevrala, S. D. Probert. Modelling convective currents in rooms by means of wall jets. Building Services Engineering Research Technology, 2(1), 1981. [Pg.1195]

The fluxing model was iniiially proposed by librhstctn and DeCrescciue, and kjes lopibd %. CBwbd s d ajiii cidhi -b ctoff... [Pg.1066]

As outlined in Section D.2.3.5., the stereochemical outcome of the addition of nucleophilic reagents to chiral aldehydes or ketones is rationalized most plausibly by the Cram-Felkin-Anh model. On the other hand, the corresponding reactions of oxygen- or nitrogen-heterosub-stituted aldehydes or ketones may be interpreted either by the same transition state hypothesis or, alternatively, by Cram s cyclic model. [Pg.563]

A prototype is a 3-D model suitable for use in the preliminary testing and evaluation of a product (also used for modeling a die, mold and other tool). It provides a means to evaluate the product s performances before going into production. The ideal situation is for the prototype to be the actual product made in production. However machining stock material and using rapid prototype techniques can make prototypes (Chapter 4, BOOK SHELVES). [Pg.178]

Miller, J., University of Utah Miller, S. D., Ampex Corporation Model, M., Modec... [Pg.212]

Grime, J.P. (1988). The C-S-R model of primary plant strategies - origins, implications and tests. In Plant Evolutionary Biology, ed. L.D. Gottlieb and K. Jain, pp. 371-93. London Chapman Hall. [Pg.44]

Sjoerdsma S.D., Bleijenberg A.C.A.M., and Heikens D., The Poisson ratio of polymer blend, effects of adhesion and correlation with the Kemer packed grain model. Polymer, 22, 619, 1981. [Pg.163]

T. Schuller, S. Ducruix, D. Durox, and S. Candel. Modeling tools for the prediction of premixed flame transfer functions. Proc. Combust. Inst., 29 107-113, 2002. [Pg.92]

Bergstrom, C. A. S. D., Norinder, U., Luthman, K., Artursson, P. Experimental and computational screening models for prediction of aqueous drug solubility. Pharm. Res. 2002, 19,182-188. [Pg.125]

However, there is still a strong need to develop new methods that will be able to quantitatively or at least qualitatively estimate the prediction accuracy of log D models. Such models will allow the computational chemist to distinguish reliable versus nonreliable predictions and to decide whether the available model is sufficiently accurate or whether experimental measurements should be provided. For example, when applying ALOGPS in the LIB RARY model it was possible to predict more than 50% and 30% compounds with an accuracy of MAE <0.35 for Pfizer and AstraZeneca collections, respectively [117]. This precision approximately corresponds to the experimental accuracy, s=0.4, of potentiometric lipophilicity determinations [15], Thus, depending on the required precision, one could skip experimental measurements for some of the accurately predicted compounds. [Pg.429]


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See also in sourсe #XX -- [ Pg.108 , Pg.110 ]




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