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Upper limit distribution

Mugele and Evans14231 proposed the upper-limit distribution function based on their analyses of various distribution functions and comparisons with experimental data. This distribution function is a modified form of the log-normal distribution function, and for droplet volume distribution it is expressed as ... [Pg.246]

The upper-limit distribution function assumes a finite minimum and maximum droplet size, corresponding to a y value of -oo and +oo, respectively. The function is therefore more realistic. However, similarly to other distribution functions, it is difficult to integrate and requires the use of log-probability paper. In addition, it usually requires many trials to determine a most suitable value for a maximum droplet size. [Pg.247]

Keywords Characteristic drop diameter Cumulative volume fraction Discrete probability function (DPF) Drop size distribution Empirical drop size distribution Log-hyperbolic distribution Log-normal distribution Maximum entropy formalism (MEF) Nukiyama-Tanasawa distribution Number distribution function Probability density function (pdf) Representative diameter Root-normal distribution Rosin-Rammler distribution Upper limit distribution Volume distribution... [Pg.479]

The upper-limit distribution is a modified version of the log-normal distribution. It is a volume distribution, and a maximum drop size is introduced ... [Pg.482]

Parameter Mean Coefficient of variation [Lower and upper limits] Distribution type... [Pg.2425]

For heavy molecules with very small rotational state spacing, this limit on AJ puts severe upper limits on the amount of energy that can be taken up in the rotations of a heavy molecule during a collision. Despite these limitations, P(E, E ) distributions have been obtained by inverting data of the type described here for values of AE in the range -1500 cm > AE > -8000 cnD for the two donor molecules pyrazine and hexafluorobenzene with carbon dioxide as a bath acceptor molecule [15,16]. Figure C3.3.11 shows these experimentally derived... [Pg.3011]

Foster s neglect of the role of the adsorbed film was unavoidable in the then absence of any reliable information as to the thickness of the film. It is now known that in fact the effect of the film on the calculated result is far from negligible, as will be demonstrated shortly. Since, however, all the methods of calculating pore size distributions involve a decision as to the upper limit of the range to be studied, this question needs to be discussed first. In effect one has to choose a point corresponding to point G in Fig. 3.1, where the mesopores are deemed to be full up. If the isotherm takes the course GH there are no further cores to be considered in any case but if it swings upwards as at GH, the isotherm is usually so steep that the Kelvin-type approach becomes too inaccurate (cf. p. 114) to be useful. [Pg.133]

Analysis. Analyses of a number of lignitic coals are given in Table 3. Figure 1, a distribution plot of 300 U.S. coals according to ASTM classification by rank, indicates the broad range of fixed carbon values (18). According to the ASTM classification, fixed carbon for both lignite and subbituminous coals has an upper limit of 69%, but in practice this value rarely exceeds 61%. [Pg.151]

Figure 5.1 The parabolic distribution in energy, N(E), as function of energy, E, for free electrons. The Fermi surface represents the upper limit of electron energy at the absolute zero of temperature, but at higher temperatures a small fraction of the electrons can be excited to higher energy levels... Figure 5.1 The parabolic distribution in energy, N(E), as function of energy, E, for free electrons. The Fermi surface represents the upper limit of electron energy at the absolute zero of temperature, but at higher temperatures a small fraction of the electrons can be excited to higher energy levels...
Water sample collection techniques differ depending on the source being tested. The minimum number of water samples collected from a distribution system which are examined each month for coliforms is a function of the population. For example, the minimum number required for populations of 1,000 and 100,000 are 2 and 100, respectively. To ascertain compliance with the bacteriological requirements of drinking water standards, a certain number of positive tests must not be exceeded. When 10-ml standard portions are examined, not more than 10 percent in any month should be positive (that is, the upper limit of coliform density is an average of one per 100 ml). [Pg.461]

For lean streams, you are asked to enter supply composition, target composition, maximum MSA flowrate, solute distribution (m), constant (b), cost, and epsilon (minimum composition difference). If an MSA has no upper limit to flowrate, enter a laige number or leave the flowrate as zero in this input held. Essentially all external MSAs fall into this category, while many internal MSAs are only available in certain quantities. [Pg.310]

Selection 2 is a similar calculation using the F-Number method (Section 2.5.3.2) 3 calculates the integral over the Chi-Squared distribution. When selected i nput the upper limit of integration... [Pg.457]

Most materials will tend to approximate log-probability distributions at the fine end (usually with standard geometric deviations in the range of 2 to 3) and to level off at some upper limiting size, as indicated by the solid curve. Approximating the data by a straight line either in the fine range or over the entire range may, at times, be expedient because of the ease with which certain properties of the material can be ascertained analytically... [Pg.497]

The integral in equation 11.55 clearly has a finite value within the thermal boundary layer, although it is zero outside it. When the expression for the temperature distribution in the boundary layer is inserted, the upper limit of integration must be altered from /... [Pg.688]

Experiments have been carried out on the mass transfer of acetone between air and a laminar water jet. Assuming that desorption produces random surface renewal with a constant fractional rate of surface renewal, v, but an upper limit on surface age equal to the life of the jet, r, show that the surface age frequency distribution function, 4>(t), for this case is given by ... [Pg.855]

Here the point p belongs to the spherical surface A of radius R. In order to find the upper limit on the left hand side of this equality, let us recall that T is the disturbing potential. In other words, it is caused by the irregular distribution of masses whose sum is equal to zero. This means that its expansion in power series with Legendre s functions does not contain a zero term. The next term is also equal to zero, because the origin coincides with the center of mass. Therefore, the series describing the function T starts from the term, which decreases as r. This means that the product r T O if oo and... [Pg.126]

Rainfall is an important criterion of climatic suitability, but precise requirements cannot be stated since its distribution pattern, atmospheric humidity, temperature, and altitude all affect plant requirements. If drainage is adequate, there does not seem to be an upper limit since tea is grown successfully in some parts of Sri Lanka where rainfall exceeds 500cm/yr.19 Long periods of drought are harmful, but are mitigated to some extent by high atmospheric humidity and lower temperatures. [Pg.51]

This value represents the upper limit of a first order reaction rate constant, k, which may be determined by the RHSE. This limit is approximately one order of magnitude smaller that of a rotating electrode. One way to extend the upper limit is to combine the RHSE with an AC electrochemical technique, such as the AC impedance and faradaic rectification metods. Since the AC current distribution is uniform on a RHSE, accurate kinetic data may be obtained for the fast electrochemical reactions with a RHSE. [Pg.201]

For solvent operations, benzene use had to be estimated by a series of tenuous assumptions about the amount of benzene in "other uses," the percent of that used for solvents, and the loss of benzene from those operations. As an upper limit, it might be assumed that all of the purchased benzene is eventually lost to the atmosphere. However, some measured concentrations suggest that perhaps only 10% is lost at the plant. The remainder might be incinerated after becoming unusable or sent elsewhere for disposal. A general rule for volatile solvents is that they eventually reach the environment unless they are destroyed deliberately or degrade naturally. The distribution of solvent emissions geographically is much more difficult to determine. [Pg.22]

Fig. 6.5. Graphical illustration of the inaccuracy model and the relative free energy error in forward and reverse free energy calculations. A limit-perturbation Xf is adopted to (effectively) describe the sampling of the distribution the regions above x/ are assumed to be perfectly sampled while regions below it shaded area) are never sampled. We may also put a similar upper limit x f for the high-rr tail, where there is no sampling for regions above it. However, this region (in a forward calculation) makes almost zero contribution to the free energy calculation and its error. Thus for simplicity we do not apply such an upper limit here... Fig. 6.5. Graphical illustration of the inaccuracy model and the relative free energy error in forward and reverse free energy calculations. A limit-perturbation Xf is adopted to (effectively) describe the sampling of the distribution the regions above x/ are assumed to be perfectly sampled while regions below it shaded area) are never sampled. We may also put a similar upper limit x f for the high-rr tail, where there is no sampling for regions above it. However, this region (in a forward calculation) makes almost zero contribution to the free energy calculation and its error. Thus for simplicity we do not apply such an upper limit here...
For a dust ignition to occur, the suspended solids concentration must lie between lower and upper limits which vary from material to material and are influenced by subtle factors such as particle shape and size distribution. From the standpoint of assessing safety hazards in commercial and industrial operations, the lower explosive limit is the more important one. The rationale of this statement is that, if the possibility of exceeding the lower limit in a powder-handling operation can not be completely ruled out, then a hazard must be recognized and appropriate measures taken. Over the... [Pg.838]

Thus the mass of stars and that of the whole system steadily increase while z soon approaches 1 and the stellar metallicity distribution is very narrow (see Fig. 8.24). The accretion rate is constant in time if the star formation rate is any fixed function of the mass of gas. Other models in which the accretion rate is constant, but less than in the extreme model, have been quite often considered in the older literature (e.g. Twarog 1980), but are less popular now because they are not well motivated from a dynamical point of view, there is an upper limit to the present inflow rate into the whole Galaxy of about 1 M0yr 1 from X-ray data (Cox Smith 1976) and they do not provide a very good fit to the observed metallicity distribution function. [Pg.277]


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See also in sourсe #XX -- [ Pg.482 , Pg.483 ]




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