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Class size

Table 1 summarizes typical data the specific breakage rate, 3), for particles in size class 1 is 0.6, and the breakage product mass in size classes 2—6 is as shown. The corresponding values of b and B are given. [Pg.139]

Using the above concepts, models have been developed to predict size distribution from comminution devices. An assumption is that the rate of breakage of material of a particular size is proportional to the mass of that size present in the comminution zone of a machine. If the mass size distribution in the machine is where is the mass of particles in size class /, then rate of breakage is given by equation 2. [Pg.139]

Thep and q denote the integral exponents of D in the respective summations, and thereby expHcitiy define the diameter that is being used. and are the number and representative diameter of sampled drops in each size class i For example, the arithmetic mean diameter, is a simple average based on the diameters of all the individual droplets in the spray sample. The volume mean diameter, D q, is the diameter of a droplet whose volume, if multiphed by the total number of droplets, equals the total volume of the sample. The Sauter mean diameter, is the diameter of a droplet whose ratio of volume-to-surface area is equal to that of the entire sample. This diameter is frequendy used because it permits quick estimation of the total Hquid surface area available for a particular industrial process or combustion system. Typical values of pressure swid atomizers range from 50 to 100 p.m. [Pg.331]

Class 125 cast iron class ISO steel, MSS-SP-42 th rough 12-in size Class 250 cast iron ... [Pg.966]

Nominal valve size Class 300 steel Class 400 steel Class 600 steel ... [Pg.966]

There are numerous machines and machine types to obtain a number of different particle-size classes from sohds having a full range of sizes, and there is much overlapping in the possibihties. Usually, one type will provide optimum economy for the specific problem involved. [Pg.1776]

This model is based on the calculation of probability p of x-ray photon impact on the j-kind particle, referred to fixed size class ... [Pg.113]

Drains shall be provided at the low points of the inlet easing and be at least 1.5 in. in size. Class 300. [Pg.309]

The level of detail GASFLOW is changed by the number of nodes, number of aero.sol particle size classes, and the models selected. It is applicable to any facility regardless of ventilation systems. It models selected rooms in detail while treating other rooms in less detail. [Pg.354]

Impactors utilize aerodynamic forces to separate the various particle size classes. This is consistent with the particles aerodynamic diameter. The operation... [Pg.1292]

All other cases are between the extreme limits of Stokes s and Newton s formulas. So we may say, that modeling the free-falling velocity of any single particle by the formula (14.49), the exponent n varies in the region 0.5 s n < 2. In the following we shall assume that k and n are fixed, which means that we consider a certain size-class of particles. [Pg.1331]

Maximum Load Rating. The maximum load ratings shall be given in tons (2,000-lb units). The size class designation shall represent the dimensional interchangeability and the maximum rated load of equipment specified herein. The recommended size classes are as follows (ton) ... [Pg.531]

As it turns out, one vendor s material contains almost no particles (0.5%) in the 261-564 /xm class (bin 15) this means that the %-weight results accurately represent the situation. The other vendor s material, however, contains a sizable fraction (typically 5%, maximally 9%) in this largest size class this implies that 1-5% invisible material is in the size class >564 /xm. Evidently then, the size distribution curve for this second material is accurate only on... [Pg.216]

Note. If the N dimensions yield very different numerical values, such as 105 3 mmol/L, 0.0034 0.02 meter, and 13200 600 pg/ml, the Euclidian distances are dominated by the contributions due to those dimensions for which the differences A-B, AS, or BS are numerically large. In such cases it is recommended that the individual results are first normalized, i.e., x = (x - Xn,ean)/ 5 t, where Xmean and Sx are the mean and standard deviation over all objects for that particular dimension X, by using option (Transform)/(Normalize) in program DATA. Use option (Transpose) to exchange columns and rows beforehand and afterwards The case presented in sample file SIEVEl.dat is different the individual results are wt-% material in a given size class, so that the physical dimension is the same for all rows. Since the question asked is are there differences in size distribution , normalization as suggested above would distort tbe information and statistics-of-small-numbers artifacts in the poorly populated size classes would become overemphasized. [Pg.371]

Saski EK, JK Jokela, MS Salkinoja-Salonen (1996a) Biodegradability of different size classes of bleached kraft mill effluent organic halogens during wastewater treatment and in lake environments. In Environmental Fate and Effects of Pulp and Paper Mill Effluents (Eds MR Servos, KR Munlittrick, JH Carey, and GJ van der Kraak), pp. 179-193. St Lucie Press, Delray Beach, FL. [Pg.275]

Sorption. Capture of neutral organics by non-living particulates depends on the organic carbon content of the solids (9). Equilibrium sorption of such "hydrophobic" compounds can be described by a carbon-normalized partition coefficient on both a whole-sediment basis and by particle size classes. The success of the whole-sediment approach derives from the fact that most natural sediment organic matter falls in the "silt" or "fine" particle size fractions. So long as dissolved concentrations do not exceed 0.01 mM, linear isotherms (partition coefficients) can be used. At higher concentrations, the sorptive capacity of the solid can be exceeded, and a nonlinear Freundlich or Langmuir isotherm must be invoked. [Pg.27]

In the case of droplets and bubbles, particle size and number density may respond to variations in shear or energy dissipation rate. Such variations are abundantly present in turbulent-stirred vessels. In fact, the explicit role of the revolving impeller is to produce small bubbles or drops, while in substantial parts of the vessel bubble or drop size may increase again due to locally lower turbulence levels. Particle size distributions and their spatial variations are therefore commonplace and unavoidable in industrial mixing equipment. This seriously limits the applicability of common Euler-Euler models exploiting just a single value for particle size. A way out is to adopt a multifluid or multiphase approach in which various particle size classes are distinguished, with mutual transition paths due to particle break-up and coalescence. Such models will be discussed further on. [Pg.170]

Venneker et al. (2002) used as many as 20 bubble size classes in the bubble size range from 0.25 to some 20 mm. Just like GHOST , their in-house code named DA WN builds upon a liquid-only velocity field obtained with FLUENT, now with an anisotropic Reynolds Stress Model (RSM) for the turbulent momentum transport. To allow for the drastic increase in computational burden associated with using 20 population balance equations, the 3-D FLUENT flow field is averaged azimuthally into a 2-D flow field (Venneker, 1999, used a less elegant simplification )... [Pg.206]

Barghigiani, C. and S. De Ranieri. 1992. Mercury content in different size classes of important edible species of the northern Tyrrhenian Sea. Mar. Pollut. Bull. 24 114-116. [Pg.425]

Green SV, Dao TH, Cavigelli MA, Flanagan DC (2006) Phosphorus fractions and dynamics among soil aggregate size classes of organic and conventional cropping systems. Soil Sci 171 874-885... [Pg.296]

The solution of the gas flow and temperature fields in the nearnozzle region (as described in the previous subsection), along with process parameters, thermophysical properties, and atomizer geometry parameters, were used as inputs for this liquid metal breakup model to calculate the liquid film and sheet characteristics, primary and secondary breakup, as well as droplet dynamics and cooling. The trajectories and temperatures of droplets were calculated until the onset of secondary breakup, the onset of solidification, or the attainment of the computational domain boundary. This procedure was repeated for all droplet size classes. Finally, the droplets were numerically sieved and the droplet size distribution was determined. [Pg.363]


See other pages where Class size is mentioned: [Pg.131]    [Pg.131]    [Pg.139]    [Pg.335]    [Pg.313]    [Pg.320]    [Pg.535]    [Pg.165]    [Pg.166]    [Pg.167]    [Pg.168]    [Pg.169]    [Pg.216]    [Pg.216]    [Pg.260]    [Pg.282]    [Pg.581]    [Pg.197]    [Pg.373]    [Pg.373]    [Pg.373]    [Pg.42]    [Pg.252]    [Pg.460]    [Pg.206]    [Pg.308]    [Pg.80]    [Pg.158]    [Pg.346]    [Pg.404]   
See also in sourсe #XX -- [ Pg.442 , Pg.616 ]




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