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Size distribution function standard deviations

Emphasis has also been placed on the particle size distribution and the uniform size distribution of the API rather than on the mean particle size alone by other authors.1416 Rohrs et al.16 give a nomograph for identifying the maximum median particle diameter to pass USP 28 stage I content uniformity criteria with 99% confidence as a function of dose as well as width of particle size distribution (geometrical standard deviation). [Pg.73]

Aerosol, monodisperse An aerosol with a size-distribution function described by a geometrical standard deviation less than 1.15. If the deviation is between 1.15 and 1.5, it is classified as a quasi-mono-disperse aerosol. [Pg.1406]

Fig. 3. Statistical models a Correlation between the product of sets sizes and the mean of the raw score. The fitted function typically corresponds to an equation of the formula = mxn + p with n = 1. b Correlation between the product of sets sizes and the standard deviation of the raw score. The fitted function typically corresponds to an equation of the formula ya=qxr+ s, with 0.6 Fig. 3. Statistical models a Correlation between the product of sets sizes and the mean of the raw score. The fitted function typically corresponds to an equation of the formula = mxn + p with n = 1. b Correlation between the product of sets sizes and the standard deviation of the raw score. The fitted function typically corresponds to an equation of the formula ya=qxr+ s, with 0.6 <r< 0.7. c Distribution of the z-scores obtained from random data using ECFP 4 fingerprints, with a similarity score threshold (t) of 0.57 and fitted to an extreme value distribution.
After n repetitive measurements of the cumulative distribution function Q of a certain particle size x the standard deviation Sq(x) from its mean Q(x) can be calculated to... [Pg.447]

In reality, the queue size n and waiting time (w) do not behave as a zero-infinity step function at p = 1. Also at lower utilization factors (p < 1) queues are formed. This queuing is caused by the fact that when analysis times and arrival times are distributed around a mean value, incidently a new sample may arrive before the previous analysis is finished. Moreover, the queue length behaves as a time series which fluctuates about a mean value with a certain standard deviation. For instance, the average lengths of the queues formed in a particular laboratory for spectroscopic analysis by IR, H NMR, MS and C NMR are respectively 12, 39, 14 and 17 samples and the sample queues are Gaussian distributed (see Fig. 42.3). This is caused by the fluctuations in both the arrivals of the samples and the analysis times. [Pg.611]

To characterize a droplet size distribution, at least two parameters are typically necessary, i.e., a representative droplet diameter, (for example, mean droplet size) and a measure of droplet size range (for example, standard deviation or q). Many representative droplet diameters have been used in specifying distribution functions. The definitions of these diameters and the relevant relationships are summarized in Table 4.2. These relationships are derived on the basis of the Rosin-Rammler distribution function (Eq. 14), and the diameters are uniquely related to each other via the distribution parameter q in the Rosin-Rammler distribution function. Lefebvre 1 calculated the values of these diameters for q ranging from 1.2 to 4.0. The calculated results showed that Dpeak is always larger than SMD, and SMD is between 80% and 84% of Dpeak for many droplet generation processes for which 2left-hand side of Dpeak. The ratio MMD/SMD is... [Pg.249]

Another aspect of matching output to user needs involves presentation of results in a statistical framework—namely, as frequency distributions of concentrations. The output of deterministic models is not directly suited to this task, because it provides a single sample point for each run. Analytic linkages can be made between observed frequency distributions and computed model results. The model output for a particular set of meteorologic conditions can be on the frequency distribution of each station for which observations are available in sufficient sample size. If the model is validated for several different points on the frequency distribution based on today s estimated emission, it can be used to fit a distribution for cases of forecast emission. The fit can be made by relating characteristics of the distribution with a specific set of model predictions. For example, the distribution could be assumed to be log-normal, with a mean and standard deviation each determined by its own function of output concentrations computed for a standardized set of meteorologic conditions. This, in turn, can be linked to some effect on people or property that is defined in terms of the predicted concentration statistics. The diagram below illustrates this process ... [Pg.698]

In this example, the likelihood function is the distribution on the average of a random sample of log-transformed tissue residue concentrations. One could assume that this likelihood function is normal, with standard deviation equal to the standard deviation of the log-transformed concentrations divided by the square root of the sample size. The likelihood function assumes that a given average log-tissue residue prediction is the true site-specific mean. The mathematical form of this likelihood function is... [Pg.61]

Fig. 11. Average highest affinity (average first-order statistic) in the initial library as a function of library size. The affinity distribution p(Ka) is log-normal with mean 3.2 x 106 M and standard deviation 107 (from Ref. 14). While the average affinity ofthe best ligand always increases with increasing library size, the incremental increase for one more library member decreases as the library is made larger. This diminishing return relates to the tradeoff in library size versus ligand copy number described in the Levitan/Kauffman model (see text). Fig. 11. Average highest affinity (average first-order statistic) in the initial library as a function of library size. The affinity distribution p(Ka) is log-normal with mean 3.2 x 106 M and standard deviation 107 (from Ref. 14). While the average affinity ofthe best ligand always increases with increasing library size, the incremental increase for one more library member decreases as the library is made larger. This diminishing return relates to the tradeoff in library size versus ligand copy number described in the Levitan/Kauffman model (see text).
The normal probability function table given in the appendix d this book can also be used for values of the log-normal distribution function, f, and the log-normal cumulative distribution function, F. In these tables Z = [ln(d/cy/(In o- )] is used. A plot of the cumulative log-normal distribution is linear on log-normal probability paper, like that shown in Figure 2.11. A size distribution that fits the log-normal distribution equation can be represented by two numbers, the geometric mean size, dg, and the geometric standard deviation,. The geometric mean size is the size at 50% of the distribution, d. The geometric standard deviation is easily obtained finm the following ratios ... [Pg.70]


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