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Parameter, defined

Material parameters defined by Equations (1.11) and (1.12) arise from anisotropy (i.e. direction dependency) of the microstructure of long-chain polymers subjected to liigh shear deformations. Generalized Newtonian constitutive equations cannot predict any normal stress acting along the direction perpendicular to the shearing surface in a viscometric flow. Thus the primary and secondary normal stress coefficients are only used in conjunction with viscoelastic constitutive models. [Pg.6]

Three parameters define the performance of a classifier. These are cut size, shaipness of cut, and eapaeity. Cut size, X50, is the size at which 50 percent of the material goes into the coarse product and 50 percent into the fine. (This should not be confused with the cutoff size, a name sometimes given to the top size of the fine product .)... [Pg.1835]

Expander effieieney is related to gas flow, enthalpy drop, and shaft rotating speed. The eombination of these parameters defines impeller blade geometries required to maximize thermal effieieney. Expander... [Pg.60]

As one eaii see, the thermal parameters define a physieally different situation. For a radial-leaded diode, the heat ean only be eondueted from the die, via the leads. The thermal resistanee would then ehange as a funetion of lead-length and is published this way in data sheets. The thermal expression (see Figure A-6a) is... [Pg.191]

With the above as an introduction, we now consider the important operational case of filtration performed under constant pressure. In practice, all the parameters defined above are nearly constant under steady state conditions except V and r, which are varied by the operator. We may therefore integrate the working expression for filtration over the limits of volume from 0 to V, and for residence time over the limits of 0 to x ... [Pg.379]

In addition, it is convenient to define the Bjerrum length parameter Lb = e z ) / f.eikTi (where is the universal dielectic constant) and the so-called quenching parameter, defined as g = EqTq/eiTi. [Pg.338]

Figure 10-114. Design chart for liquid volume fraction using parameter defined in equation 10-168. (Used by permission Fair, J. R. Petroleum Refiner, Feb. 1960, p. 105. Gulf Publishing Company. All rights reserved.)... Figure 10-114. Design chart for liquid volume fraction using parameter defined in equation 10-168. (Used by permission Fair, J. R. Petroleum Refiner, Feb. 1960, p. 105. Gulf Publishing Company. All rights reserved.)...
R is the distance parameter, defining the upper limit of ion association. For spherical ions forming contact ion pairs it is simply the sum of the crystallographic radii of the ions a — a+ + a for solvent-shared and solvent-separated ion pairs it equals a + s or a + 2s respectively, where s is... [Pg.466]

R distance parameter defining upper limit of ion association III.7... [Pg.597]

Here, x and y are the dimensionless distance and potential defined by x = xr and y = e

elementary charge, T the absolute temperature, k the Boltzmann constant, and x the Debye screening parameter defined by x = (8jtne2/skT)1/2. [Pg.56]

Then, in this two-term unfolding model remains to define this exponent 2q, since all other quantities and especially the r-radius are either given, or evaluated from the thermodynamic equilibrium relations. Then, in this model the 2q-exponent is the characteristic parameter defining the quality of adhesion and therefore it may be called the adhesion coefficient. This exponent depends solely on the ratios of the main-phase moduli (Ef/Em), as well as on the ratio of the radii of the fiber and the mesophase. [Pg.163]

The critical value of the Reynolds number (Remit) for the transition from laminar to turbulent flow may be calculated from the Ryan and Johnson001 stability parameter, defined earlier by equation 3.56. For a power-law fluid, this becomes ... [Pg.138]

Here x is the polymer-solvent interaction parameter defined by Flory for polymeric swelling its value becomes more negative as the interaction between the solvent and the polymer increases. By comparing Eqs. (45) and (46), we arrive at... [Pg.402]

Tables IV and V contain appropriate balance equations for nonisothermal free-radical polymerizations and copolymerizations, which are seen to conform to equation 2k. Following the procedure outlined above, we obtain the CT s for homopolymerizations listed in Table VI. Corresponding CT s for copolymerizations can be. obtained in a similar way, and indeed the first and fourth listed in Table VII were. The remaining ones, however, were derived via an alternate route based upon the definitions in Table VI labeled "equivalent" together with approximate forms for pj, which were necessitated by application of the Semenov-type runaway analysis to copolymerizations, and which will subsequently be described. Some useful dimensionless parameters defined in terms of these CT s appear in Tables VIII, IX and X. Tables IV and V contain appropriate balance equations for nonisothermal free-radical polymerizations and copolymerizations, which are seen to conform to equation 2k. Following the procedure outlined above, we obtain the CT s for homopolymerizations listed in Table VI. Corresponding CT s for copolymerizations can be. obtained in a similar way, and indeed the first and fourth listed in Table VII were. The remaining ones, however, were derived via an alternate route based upon the definitions in Table VI labeled "equivalent" together with approximate forms for pj, which were necessitated by application of the Semenov-type runaway analysis to copolymerizations, and which will subsequently be described. Some useful dimensionless parameters defined in terms of these CT s appear in Tables VIII, IX and X.
There are two approaches for strueture optimization de-sign> parametric optimization and topology optimization. The parametric optimization aims at attaining the best set of geometric or structural parameters defining the configura-... [Pg.111]


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See also in sourсe #XX -- [ Pg.143 ]




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