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Residence times frequency distributions

Fig. lO-l. Curves illustrating the residence time distribution F(l), residence time decay function R l), and residence time frequency function / (/) for a CSTR. [Pg.372]

Since the foundations of residence time theory are rigorously given elsewhere (5,6, 7), only those features which are essential to the present treatment will be given here. The residence time distribution (residence time frequency function exit age distribution), f(t), is defined such that f(t)dt is the fraction of fluid at any instant leaving the system, having spent time between t and t + dt within the system. The cumulative residence time distribution is... [Pg.205]

The deposition velocities depend on the size distribution of the particulate matter, on the frequency of occurrence and intensity of precipitation, the chemical composition of the particles, the wind speed, nature of the surface, etc. Typical values of and dj for particles below about 1 average residence time in the atmosphere for such particles is a few days. [Pg.81]

It is normally called the differential distribution function (of residence times). It is also known as the density function or frequency function. It is the analog for a continuous variable (e.g., residence time i) of the probabiUty distribution for a discrete variable (e.g., chain length /). The fraction that appears in Equations (15.2), (15.3), and (15.6) can be interpreted as a probability, but now it is the probability that t will fall within a specified range rather than the probability that t will have some specific value. Compare Equations (13.8) and (15.5). [Pg.542]

It has been shown recently [25] that concentrations of NOj, tend to reduce with increase in the amplitude of discrete-frequency oscillations. The mechanisms remain uncertain, but may be associated with the imposition of a near-sine wave on a skewed Gaussian distribution with consequent reduction in the residence time at the adiabatic flame temperature. Profiles of NO, concentrations in the exit plane of the burner are shown in Fig. 19.6 as a function of the amplitude of oscillations with active control used to regulate the amplitude of pressure oscillations. At an overall equivalence ratio of 0.7, the reduction in the antinodal RMS pressure fluctuation by 12 dB, from around 4 kPa to 1 kPa by the oscillation of fuel in the pilot stream, led to an increase of around 5% in the spatial mean value of NO, compared with a difference of the order of 20% with control by the oscillation of the pressure field in the experiments of [25]. The smaller net increase in NO, emissions in the present flow may be attributed to an increase in NOj due to the reduction in pressure fluctuations that is partly offset by a decrease in NOj, due to the oscillation of fuel on either side of stoichiometry at the centre of the duct. [Pg.304]

Not only must we optimize the expression and yield of purified recombinant proteins, we must ensure that the protein is stable, has a high degree of potency and a low degree of toxicity, and has suitable pharmaceutical properties. Pharmaceutical properties encompass distribution and residence time in target tissues, and frequency of dosing, and may have an impact on efficacy and safety. [Pg.51]

In this section, we restrict our analysis to the second step of this procedure. The nomenclature we use is as follows Cp(x) is the concentration distribution in the feed to any given reactor, normalized so that = = 1, and Ce(x) is the corresponding distribution in the product stream. Let C = is the overall residue. Finally, let Tbe the dimensionless residence time in the reactor, that is, the actual residence time times the average value of the frequency factor in the feed mixture. [Pg.50]

We now move to the consideration of reactors with an assigned residence time distribution (RTD)y(O. where t is the dimensionless residence time (i.e., the dimensional one times the average frequency factor in the feed). In this section, we indicate with curly braces integrals over t ranging from 0 to < . Then [/(t) = 1 and T = [tj t). We also make use of the complementary cumulative RTD, F(t), which is defined as... [Pg.52]

Rate of growth (low deformability) Increase rate of nuclei formation. Increase collision frequency. Increase residence time. Improve wetting properties. (See Wetting subsection.) Increase binder distribution. Increase spray rate and number of drops. Increase mixer impeller or drum rotation speed or fluid-bed gas velocity. Increase batch time or lower feed rate. [Pg.2358]


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See also in sourсe #XX -- [ Pg.365 , Pg.367 , Pg.372 , Pg.373 ]




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