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Deviations distribution

A function of a random sample of data (e.g. mean, standard deviation, distribution parameters). [Pg.102]

Figure 1. Log-normal distributions used to create a bimodal-distribution model of a hypothetical rubber-toughened plastic. Distribution 1 2.0-pm average diameter, 0.4-pm standard deviation. Distribution 2 8.0-pm average diameter 0.8-pm standard deviation. Figure 1. Log-normal distributions used to create a bimodal-distribution model of a hypothetical rubber-toughened plastic. Distribution 1 2.0-pm average diameter, 0.4-pm standard deviation. Distribution 2 8.0-pm average diameter 0.8-pm standard deviation.
The three normal distributions in Figure 28.11 have the same mean but different standard deviations. Distribution A has the highest standard deviation because it is the fattest. Distribution C has the lowest and... [Pg.372]

The spatial and temporal damping due to simultaneous dissipation and deviated distribution. [Pg.587]

These equations model the spatial and temporal damping due to simultaneous dissipation and deviated distribution, which is one of the kinds of damping. The two other kinds are ... [Pg.590]

Fig. 11.13 Behaviour of the bridging oxygen centred standard deviation distributions f(cr) in a NS2 liquid. Note the bimodal distribution occuring at T 2000 K. The broken line defines a boundary between broken and intact constraints, estimated to be about erg = 15° at low temperature. Gaussian fits red curves) are shown for selected temperatures.The inset shows the fraction q(T) of intact BO constraints as a function of temperature. The solid curve is a fit using the Mauro-Gupta function [37]... Fig. 11.13 Behaviour of the bridging oxygen centred standard deviation distributions f(cr) in a NS2 liquid. Note the bimodal distribution occuring at T 2000 K. The broken line defines a boundary between broken and intact constraints, estimated to be about erg = 15° at low temperature. Gaussian fits red curves) are shown for selected temperatures.The inset shows the fraction q(T) of intact BO constraints as a function of temperature. The solid curve is a fit using the Mauro-Gupta function [37]...
Fig. 11.18 a Behaviour of the bridging oxygen centred angular standard deviation distributions Rct) in aNS2 liquid at 2000 K as a function or pressure, b Isobaric fraction q(Po,T) of intact angular (BB) constraints for different isobars in simulated NS2 liquids (symbols). The lines represent least-squares fit using the Mauro-Gupta function [37]... [Pg.301]

The ternary diagrams shown in Figure 22 and the selectivi-ties and distribution coefficients shown in Figure 23 indicate very good correlation of the ternary data with the UNIQUAC equation. More important, however, Table 5 shows calculated and experimental quarternary tie-line compositions for five of Henty s twenty measurements. The root-mean-squared deviations for all twenty measurements show excellent agreement between calculated and predicted quarternary equilibria. [Pg.76]

There are two types of measurement errors, systematic and random. The former are due to an inherent bias in the measurement procedure, resulting in a consistent deviation of the experimental measurement from its true value. An experimenter s skill and experience provide the only means of consistently detecting and avoiding systematic errors. By contrast, random or statistical errors are assumed to result from a large number of small disturbances. Such errors tend to have simple distributions subject to statistical characterization. [Pg.96]

In the maximum-likelihood method used here, the "true" value of each measured variable is also found in the course of parameter estimation. The differences between these "true" values and the corresponding experimentally measured values are the residuals (also called deviations). When there are many data points, the residuals can be analyzed by standard statistical methods (Draper and Smith, 1966). If, however, there are only a few data points, examination of the residuals for trends, when plotted versus other system variables, may provide valuable information. Often these plots can indicate at a glance excessive experimental error, systematic error, or "lack of fit." Data points which are obviously bad can also be readily detected. If the model is suitable and if there are no systematic errors, such a plot shows the residuals randomly distributed with zero means. This behavior is shown in Figure 3 for the ethyl-acetate-n-propanol data of Murti and Van Winkle (1958), fitted with the van Laar equation. [Pg.105]

The points are within the stated standard deviation and are randomly distributed about the zero axis. [Pg.106]

The method allows variables to be added or multiplied using basic statistical rules, and can be applied to dependent as well as independent variables. If input distributions can be represented by a mean, and standard deviation then the following rules are applicable for independent variables ... [Pg.168]

Of course, under the same operating conditions, the higher the thickness the lower the stress level. Further tests were carried out to map the surface thickness distribution using an ultrasonic precision thickness gauge. It was so verified a deviation of the thickness up to 10% of the nominal value. [Pg.411]

BAM produces and distributes calibrating films for the measurement of the standard deviation of the density. [Pg.554]

Although a seemingly odd mathematical entity, it is not hard to appreciate that a simple one-dimensional realization of the classical P x , t) can be constructed from the familiar Gaussian distribution centred about x by letting the standard deviation (a) go to zero. [Pg.6]

In the case of bunolecular gas-phase reactions, encounters are simply collisions between two molecules in the framework of the general collision theory of gas-phase reactions (section A3,4,5,2 ). For a random thennal distribution of positions and momenta in an ideal gas reaction, the probabilistic reasoning has an exact foundation. Flowever, as noted in the case of unimolecular reactions, in principle one must allow for deviations from this ideal behaviour and, thus, from the simple rate law, although in practice such deviations are rarely taken into account theoretically or established empirically. [Pg.769]

The velocity distribution/(v) depends on the conditions of the experiment. In cell and trap experiments it is usually a Maxwell-Boltzmann distribution at some well defined temperature, but /(v) in atomic beam experiments, arising from optical excitation velocity selection, deviates radically from the nonnal thennal distribution [471. The actual signal count rate, relates to the rate coefficient through... [Pg.2476]

The first application of the Gaussian distribution is in medical decision making or diagnosis. We wish to determine whether a patient is at risk because of the high cholesterol content of his blood. We need several pieces of input information an expected or normal blood cholesterol, the standard deviation associated with the normal blood cholesterol count, and the blood cholesterol count of the patient. When we apply our analysis, we shall anive at a diagnosis, either yes or no, the patient is at risk or is not at risk. [Pg.17]

The assumption that the deviations are randomly distributed about analytical form. [Pg.59]

We have already found that the probability function governing observation of a single event x from among a continuous random distribution of possible events x having a population mean p and a population standard deviation a is... [Pg.60]

For a specified mean and standard deviation the number of degrees of freedom for a one-dimensional distribution (see sections on the least squares method and least squares minimization) of n data is (n — 1). This is because, given p and a, for n > 1 (say a half-dozen or more points), the first datum can have any value, the second datum can have any value, and so on, up to n — 1. When we come to find the... [Pg.70]


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See also in sourсe #XX -- [ Pg.102 ]




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