Growth curves delay

Figure 1. Multiple Quantum NMR pulse. Growth curves are obtained by incrementing either the interpulse delays or the number of multiple pulse excitation trains in the conversion and reconversion sequences. (Reproduced from reference 13. Copyright 2005 American Chemical Society.)...

In part B, supersaturation is low and the distribution curve is broad, since induction times are spread over the whole aggregation delay. Thus, the autocatalytic character is lost in the resultant kinetics. According to the width of the induction time distribatior , flat or irregular curves can be obtained (Figure 10).It is a region of random growth of the domains. 

Figure 29 Model sulfur isotopic evolution in the course of geologic history. The lower trend (labeled 6 Sred) represents the for sulfides. The upper curves (labeled 6 Sox) are the of marine sulfates. TML and VJ simulations assume a logistic type of continental growth as proposed by Taylor and McLennan (1985) and Veizer and Jansen (1979), respectively. BB simulation assumes an instantaneous generation of continental crust, BB-evol simulation assumes instantaneous continental generation, but with delayed invention of oxygen generating photosynthesis. The Phanerozoic trend as in Figure 30. Dots represent measurements of Precambrian sulfates (Claypool et al, 1980) and the hatched field represents sulfates from Holser et al. (1988) (after Godderis...

First we fix ko and observe the density as a function of t for different x values. Figure 9.7 shows the density at the transition versus tp. The curve depends parametrically on x, which increases from the bottom right comer upward. From this figure we can infer that the probability density at the transition point increases, as the observation point is moved away from the source, improving the possibility of observing the transition. A basic reason for this is the asymptotic growth of I with x, whereas the pole term is basically shifted by Sx/lkoR for a shift Sx in the observation coordinate in other words, the exponential behavior is delayed by increasing x. 

The change in the shape of this curve under the influence of s.a.s. has been determined in this case through an analysis of the initial period of the drop life (first seven steps) and of the final fraction generated in the last thirteen steps. Table 2 presents experimental data taken from i-t curves for cadmium. Current samples were taken with 150 ms delay after the drop growth was stopped. The ON pulse times were 10 ms. In these experiments the starting conditions were determined by pure 1 M KNO3 as the supporting electrolyte. 

The Li-ion power tool packs exhibited a fire development trend similar to the CUP commodity. A delay in fire growth occurred at 55 s as the flames penetrated the cartons and the plastic components of the battery packs became involved in the fire. This delay was observed as a temporary plateau in the heat release curve from 55 to 75 s. The fire then grew steadily from 75 s until the lire reached a maximum of 1,900 kW. The fire size then decreased to approximately 1,250 kW, remained steady, and then decreased as a majority of the combustibles were consumed. 

The authors made many attempts to obtain points off of the calibration curve with the upstream static pressure greater than the vapor pressure and the downstream static pressure lower than the vapor pressure. In spite of the fact that the downstream static pressure was as much as 10 inches Hg below the vapor pressure, all of the points fell on the calibration curve, within the accuracy of the experiments. It is therefore probable that the time required for the nucleation and growth of bubbles in both nitrogen and hydrogen is so long that errors in the measurement of flow with sharp-edged orifices, arising from low downstream pressures, probably will not occur. This delay in vaporization downstream of an orifice has been repeatedly observed for water and other fluids, e. g., Benjamin and Miller. 

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