Fp function

The use of the exception clause traps errors in any of the isosmiles, cansmiles, or fp functions. The creation of the error log table is shown above to contain these errors for later inspection and correction. 

Comparison of the Fp functions corresponding to nonisothermal and isothermal cases shows distinctive differences in the shapes of the amplimdes of the second-order functions. The differences in the first-order functions also exist, but they become more obvious if they are shown in the form of real and imaginary parts the imaginary part of Fi p(w) for isothermal case has one minimum, while for the nonisothermal case a curve with two minima is obtained [54,59]. Also, for the case of variable micropore diffusivity, the low- and high-frequency asymptotic values of F2,pp([Pg.309]

Similar to the previous case, the derivatives of the adsorption isotherm with respect to pressure are directly related to the low-frequency limiting values of the corresponding Fp functions ... 

FIGURE 7.20 The effect of CS/FPS ratio on cadmium uptake capacity (qcd(ii)) and surface area (SA) of SOL-AD-I FPS functional precursor silane CS cross-linking silane. (From J. S. Lee, S. Gomez-Salazar, and L. L. Tavlarides. Reactive and Functional Polymers 49 159-172, 2001. With permission.)... 

The factors fp and fj have not been applied to installation costs because installation costs are not a simple function of purchase cost. Although process piping and fittings made for the same unusual conditions are proportionally more expensive, labor, foundations, insulation, etc. are not. Furthermore, only about 70 percent of piping is directly exposed to process fluid. The balance is auxiliary or utility piping made of conventional materials. 

Although magma density is a function of the kinetic parameters fP and G, it often can be measured iadependentiy. In such cases, it should be used as a constraint ia evaluating nucleation and growth rates from measured crystal size distributions (62), especially if the system of iaterest exhibits the characteristics of anomalous crystal growth. 

Figure 1. The energy of bcc and hep randoiri alloys and the ])ai tially ordered a phase relative to the energy of the fee phase (a), of the Fe-Co alloy as a function of Co concentration. The corresponding mean magnetic moments are shown in (h). The ASA-LSDA-CPA results are shown as a dashed line for the o ])hase, as a full line for the her ]>hase, as a dot-dashed line for the hep phase, and as a dotted line for the fee phase. The FP-GGA results for pure Fe and Co are shown in (a) by the filled circles (bcc-fcc) and triangles (hep-fee). In (b) experimental mean magnetic moments are shown as open circles (bcc), open scpiares (fee) and open triangles (hep).

Figure 1. The effective pair interactions as functions of alloy composition for the alloy system Al-Ni. The results of the CWIS based on the FP-LAPW calculations for 5 ordered structures (full line) and on the TB-LMTO-CPA for 5 disordered alloys (dash line) are compared with the the results of the GPM (dotted line).

The one-particle distribution function fp specifies both the total particle density p and momentum density pu, where u is the average fluid velocity. 

Rheological experiments have shown that the relative viscosity of compositions filled with the above materials is an exponential function of filler content by volume. The impact of an otherwise constant quantity of filler increases in the series FP — LDP — SDP, i.e., symbatically with the probability of particle comminution in the plasticization process. This effect is most clearly apparent for... 

The point of the weighting function can be illustrated by considering the two extremes of complete scrambling (for which ) = 1), and complete routing (forwhich f() = 1/Fp). If we choose to make f(F) = F ,we have constructed a convenient function that can be adjusted to take intermediate values (for this particular DIFF), where CO may take any values between 0 (where f(F) = 1 scrambling) and -1 (where f(F) = 1/F direct routing). Later (Section 4) we use an alternative formulation, in which... 

The constraints due to filler particles are somewhat more complicated to mimic analytically. A crude model is to assume solid spheres of an average functionality fp (—4) [15]. If... 

In POLYM the output data of KINREL are used with compositional information to calculate the number and mass average molecular masses (Rn and Rm, respectively) and number and end-group average functionalities (fp and fg> respectively) in the pre-gel region in all stages. In addition, the network characteristics such as sol fraction, mj, and the number of elastically active network chains per monomer (5), Ng, are calculated in the post-gel regime of stage 3. 

Figure 14a-c shows the variation in the Fp, the and the of a CH4/CO/H2 plasma with [CO]. While the and increase with increasing [CO], the decreases with increasing [CO]. Figure 15a-c shows the EEDFs of a CH4/CO/H2 plasma as a function of [CO]. The hump at eV still appears with the addition of CO, and the spectrum shape retains almost the same feature. The inclinations below 6 eV become slow with increasing [CO], which means that the Tg increases with increasing [CO]. It is consistent with the result of Figure 14b. The electron impact dissociation of CO produces 0 (CO + e C + 0 )ina CH4/CO/H2 plasma. It is therefore assumed that the increase in negative ions reduces the relatively to satisfy the charge balance in a plasma, and that the decrease in leads to the increase in Fp and T. ...

Fowler SW, Carvalho FP. 1985. Americium biokinetics in benthic organisms as a function of feeding mode. Bull Environ Contain Toxicol 35 826-834. 

The function Fp, which is a dimensionless or reduced bonding force, has been displayed graphically by Pietsch and Rumpf (P6) for various sets of variable p and parameters 0 and l/Dp. The volume of the liquid in the pendular bridge K is given by... 

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