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Loads equations, comparison

Because the heat load, L, Ga and temperatures are known for an operating tower, its performance as represented by the number of transfer units, or tower characteristics can be determined. Solve Equation 9-129 for Ka V/L, or use the modified Merkel diagram, Figure 9-127. This is the number of transfer units operating in the tower. For relative comparison of Ka values see Figure 9-128. [Pg.396]

Equation 27 can be numerically integrated along the conversion trajectory to obtain the Initiator concentration as function of time. Therefore, calculation of t, 6 and C together with the values of M, Rp, rw and rn from the equations In Table II allows the estimation of the ratios (ktc/kp1), (kx/kp) and the efficiency as functions of conversion. Figure 3 shows the efficiency as function of conversion. Figure 4 shows the variation of the rate constants and efficiencies normalized to their initial values. The values for the ratio (ktc/kpl)/(ktc/kpl)o reported by Hui (18) are also shown for comparison. From the definition of efficiency it is possible to derive an equation for the instantaneous loading of initiator fragments,... [Pg.211]

Figure 2. Comparison between mean film thickness of falling and agitated films in a thin-film apparatus, expressed as a function of peripheral load and viscosity. Curves I, 2, and 3, falling film according to Equation 1 curve 1° and 2°, agitated film in the thin-film apparatus... Figure 2. Comparison between mean film thickness of falling and agitated films in a thin-film apparatus, expressed as a function of peripheral load and viscosity. Curves I, 2, and 3, falling film according to Equation 1 curve 1° and 2°, agitated film in the thin-film apparatus...
A comparison of Equations (3) and (4) shows that, in both equations, the amounts of released drug are directly dependent on the area of the device, the square root of the time t, the drug-loading concentration C0, the respective saturated drug concentrations, and the drug diffusion coefficients. In addition, the release rate (the time derivate of the amount of released material) depends on the square root of time and can be stated as... [Pg.1199]

Figure 10.1 Comparison of band profiles derived from the Houghton and the Haarhoff-Van der Linde equations. Parabolic isotherm q = 20C(1 5C). L = 25 cm F = 0.25 fp = 200 s N = 12,500 theoretical plates. Loading factor 1%. 1, convex-upward isotherm 2, convex-downward isotherm. The Houghton profiles are identified by squares. The masses lost by the Houghton profiles are 5.3% and -4.5%, respectively. Reproduced with permis-sionfrom S. Golshan-Shirazi and G. Guiochon, J. Chromatogr., 506 (1989) 495 (Fig. 2). Figure 10.1 Comparison of band profiles derived from the Houghton and the Haarhoff-Van der Linde equations. Parabolic isotherm q = 20C(1 5C). L = 25 cm F = 0.25 fp = 200 s N = 12,500 theoretical plates. Loading factor 1%. 1, convex-upward isotherm 2, convex-downward isotherm. The Houghton profiles are identified by squares. The masses lost by the Houghton profiles are 5.3% and -4.5%, respectively. Reproduced with permis-sionfrom S. Golshan-Shirazi and G. Guiochon, J. Chromatogr., 506 (1989) 495 (Fig. 2).
In order to obtain more definitive information about the failure of PMMA we conducted zero-tension sinusoidal fatigue tests at 0.164 Hz l.e., p -f q In equation (4) and the peak stress Is p + q. The results are shown In Table II. Figure 2 shows the comparison of the average times to break with those predicted from equation (5) and the value of B determined from constant stress tests. As can be seen, the predicted times to fall vs. peak stress form a line nearly. parallel to the dead load data and at approximately seven fold greater failure times. The experimental results, however, are lower than the predicted values and show a concave deviation from the predicted values. [Pg.334]

For comparison of load-deflection curves, real load (P) was converted to an equivalent load (Ptq) to remove the thickness effect of tested specimens by the following equation ... [Pg.448]

A weak point of a decomposition as in Equation (8.2) is that the singular value decomposition of the matricized array is not the same for the A-, B- and C-loadings, so that, for example, a comparison of the first component for different modes as in Figure 8.23 becomes meaningless. [Pg.198]

On photolysis, co-polymers of vinyl(methylcymantrene) with octyl methacrylate have been shown to lose CO and generate polymers 45 possessing 16-electron Mn centers, which coordinate to N2 to yield 46 (Equation (16)). The coordination is reversible and can be used to prepare membranes that exhibit facilitated transport of this gas. Comparison of the diffusion coefficient for normal Henry-mode diffusion and the facilitated Langmuir-mode diffusion, due to the mediation of the manganese centers which function as N2 carriers, showed that the latter mechanism contributes substantially. Moreover, as expected for this interpretation, the contribution from the facilitated transport mode increased as the loading of the Mn sites became higher. [Pg.312]


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