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Scaling of the parameters

Discuss the relation between transforming the matrix X VlX into a correlation type matrix and scaling of the parameters. [Pg.161]

According to (5.44) the semi-logarithmic sensitivity coefficients show the local change in the solutions when the given parameter is perturbed by unity on the logarithmic scale and are invariant under the scaling of the parameters. [Pg.282]

The existence of an optimal value of y can be better understood by considering the scaling of the parameters of interest. Equation 38.28 shows that the maximum sample concentration is proportional to y ... [Pg.1100]

The detailed design of a tray is beyond the scope of this text. It involves the use of a host of semiempirical correlations and it is best to draw on information provided by vendors. The reader should, however, have a sense of scale of the parameters involved, which we attempted to provide in Table 7.4. The choice of tray is assisted by Table 7.5, which summarizes the principal features of the three major types. The scale of column dimensions is conveyed by Table 7.6. [Pg.357]

The efficiency of any search routine can be sensitive to the scaling of the parameters. Ordinarily, it is desirable to have all parameters of the same order of magnitude. Unfortunately, relaxation times and relaxation strengths generally vary over several orders of magnitude. A change of variables that helps scale the parameters... [Pg.129]

Figure C2.5.2. Scaling of the number of MBS C(MES) (squares) is shown for the hydrophobic parameter = -0.1 and A = 0.6. Data were obtained for the cubic lattice. The pairs of squares for each represent the quenched averages for different samples of 30 sequences. The number of compact stmctures C(CS) and self-avoiding confonnations C(SAW) are also displayed to underscore the dramatic difference of scaling behaviour of C(MES) and C(CS) (or C(SAW)). It is clear that C(MES) remains practically flat, i.e. it grows no faster than In N. Figure C2.5.2. Scaling of the number of MBS C(MES) (squares) is shown for the hydrophobic parameter = -0.1 and A = 0.6. Data were obtained for the cubic lattice. The pairs of squares for each represent the quenched averages for different samples of 30 sequences. The number of compact stmctures C(CS) and self-avoiding confonnations C(SAW) are also displayed to underscore the dramatic difference of scaling behaviour of C(MES) and C(CS) (or C(SAW)). It is clear that C(MES) remains practically flat, i.e. it grows no faster than In N.
This complex Ginzburg-Landau equation describes the space and time variations of the amplitude A on long distance and time scales detennined by the parameter distance from the Hopf bifurcation point. The parameters a and (5 can be detennined from a knowledge of the parameter set p and the diffusion coefficients of the reaction-diffusion equation. For example, for the FitzHugh-Nagumo equation we have a = (D - P... [Pg.3066]

The physical parameters that determine under what circumstances the BO approximation is accurate relate to the motional time scales of the electronic and vibrational/rotational coordinates. [Pg.65]

Scale- Up of Electrochemical Reactors. The intermediate scale of the pilot plant is frequendy used in the scale-up of an electrochemical reactor or process to full scale. Dimensional analysis (qv) has been used in chemical engineering scale-up to simplify and generalize a multivariant system, and may be appHed to electrochemical systems, but has shown limitations. It is best used in conjunction with mathematical models. Scale-up often involves seeking a few critical parameters. Eor electrochemical cells, these parameters are generally current distribution and cell resistance. The characteristics of electrolytic process scale-up have been described (63—65). [Pg.90]

A parameter indicating whether viscoelastic effects are important is the Deborah number, which is the ratio of the characteristic relaxation time of the fluid to the characteristic time scale of the flow. For small Deborah numbers, the relaxation is fast compared to the characteristic time of the flow, and the fluid behavior is purely viscous. For veiy large Deborah numbers, the behavior closely resembles that of an elastic solid. [Pg.631]

The electrostatic free energy contribution in Eq. (14) may be expressed as a thennody-namic integration corresponding to a reversible process between two states of the system no solute-solvent electrostatic interactions (X = 0) and full electrostatic solute-solvent interactions (X = 1). The electrostatic free energy has a particularly simple form if the thermodynamic parameter X corresponds to a scaling of the solute charges, i.e., (X,... [Pg.140]

When using dimensional analysis in computing or predicting performance based on tests performed on smaller-scale units, it is not physically possible to keep all parameters constant. The variation of the final results will depend on the scale-up factor and the difference in the fluid medium. It is important in any type of dimensionless study to understand the limit of the parameters and that the geometrical scale-up of similar parameters must remain constant. [Pg.127]

One of the more difficult decisions to be made is the proper value for the Lennard-Jones parameters. These relate to the interaction between the quantum mechanical atoms and the MM atoms. At the time of writing (1999), there does not appear to be a consensus amongst researchers. Some authors recommend a 10% scaling of the traditional 12-6 parameters. Some authors scale the MM atom charges. [Pg.263]

The scales of the various parameters should be comparable. Large differences in scale can lead to problems in fitting convergence. [Pg.237]

The ratio (p/G) has the units of time and is known as the elastic time constant, te, of the material. Little information exists in the published literature on the rheomechanical parameters, p, and G for biomaterials. An exception is red blood cells for which the shear modulus of elasticity and viscosity have been measured by using micro-pipette techniques 166,68,70,72]. The shear modulus of elasticity data is usually given in units of N m and is sometimes compared with the interfacial tension of liquids. However, these properties are not the same. Interfacial tension originates from an imbalance of surface forces whereas the shear modulus of elasticity is an interaction force closely related to the slope of the force-distance plot (Fig. 3). Typical reported values of the shear modulus of elasticity and viscosity of red blood cells are 6 x 10 N m and 10 Pa s respectively 1701. Red blood cells typically have a mean length scale of the order of 7 pm, thus G is of the order of 10 N m and the elastic time constant (p/G) is of the order of 10 s. [Pg.88]

Erom the previous sections it is clear that there are a number of different possible models that can be applied to the contact of an elastic sphere and a flat surface. Depending on the scale of the objects, their elasticity and the load to which they are subjected, one particular model can be more suitably applied than the others. The evaluation of the combination of relevant parameters can be made via two nondimensional coordinates X and P [16]. The former can be interpreted as the ratio of elastic deformation resulting from adhesion to the effective range of the surface forces. The second parameter, P, is the load parameter and corresponds to the ratio of the applied load to the adhesive puU-off force. An adhesion map of model zones can be seen in Figure 2. [Pg.21]

Since the contributions of the three constiments of the van der Waals attraction are additive, one can consider each contribution separately. This indeed proves to be convenient not only because all the contributions exhibit distinct scaling with the parameters, but each contribution comes to dominate the expansivity at somewhat distinct temperatures. We consider first the ripplon-ripplon attraction. This contribution appears to dominate the most studied region around 1 K. The off-diagonal (flip-flop) interaction between the ripplons has the form... [Pg.182]

A relative scale of the standard Gibbs energies of ion transfer or the standard ion transfer potentials can be established based on partition and solubility measurements. The partition eqnilibrium of the electrolyte can be characterized by a measnrable parameter, the partition coefficient P x-... [Pg.611]

Once the equation was well founded it became a tool for establishing a scale of resonance parameters based uniformly on infrared intensities, and particularly for measuring values of substituents which had not been obtained in other ways. It should, of course, be noted that the above equation could not give the sign of for any given substituent, since... [Pg.515]


See other pages where Scaling of the parameters is mentioned: [Pg.155]    [Pg.38]    [Pg.276]    [Pg.155]    [Pg.38]    [Pg.276]    [Pg.1210]    [Pg.2368]    [Pg.260]    [Pg.33]    [Pg.67]    [Pg.275]    [Pg.388]    [Pg.226]    [Pg.378]    [Pg.283]    [Pg.130]    [Pg.515]    [Pg.223]    [Pg.427]    [Pg.513]    [Pg.43]    [Pg.141]    [Pg.112]    [Pg.116]    [Pg.129]    [Pg.187]    [Pg.287]    [Pg.190]    [Pg.242]    [Pg.662]    [Pg.10]    [Pg.69]    [Pg.441]   
See also in sourсe #XX -- [ Pg.155 ]




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Evidence of the Interfacial Parameter Scale

Parameter scale

Scaling parameters

The 6 scale

The parameters

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