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Representation of Distribution

Heat or contaminant. sources can also be assigned to parts of the fluid volume to account for very small real sources or a distribution of a large number of small sources. Care must be taken, however, to make sure that this representation of distributed sources describes correctly the real situation (see the earlier section Geometric Modeling ). [Pg.1037]

In the same way, spatial resolving power is a measure of the efficiency of distribution-analytical methods in micro- and surface analysis as well as scanning methods. From all the systematic representations of distribution-analytical problems given in Danzer et al. [1991], the mostly relevant are represented in Fig. 7.12. [Pg.235]

FIGURE 6.4 Conceptual representation of distribution of air, LNAPL, and water in a porous media. (After Farr et al., 1990.)... [Pg.173]

Mass respirable sampling, 125 Mathematical representation of distributions, 19-24... [Pg.199]

Figure 1.4. Schematic representation of distribution of electrons in the energy bands of conductors, intrinsic semiconductors and insulators (inner levels have been omitted for clarity). VB - valence band CB - conduction band. Figure 1.4. Schematic representation of distribution of electrons in the energy bands of conductors, intrinsic semiconductors and insulators (inner levels have been omitted for clarity). VB - valence band CB - conduction band.
Figure 4.5 Diagram representation of distribution and density functions. Figure 4.5 Diagram representation of distribution and density functions.
Figure 5 Schematic representation of distribution of ions and charges in the interfacial region between a metal and an aqueous electrolyte. Figure 5 Schematic representation of distribution of ions and charges in the interfacial region between a metal and an aqueous electrolyte.
The representation of distributed wall friction for aU flow regimes from laminar to fully turbulent is required to be mathematically continuous. If this requirement is not met, then artificial modes of instability can be introduced all discontinuities present potential for introduction of instability. For sufficiently low flow rates, the changes in the fluid viscosity as the temperature changes round the loop can introduce laminar and turbulent friction flow regimes. [Pg.514]

The continuous line in Figure 16 shows results from fitting a single tie line in addition to the binary data. Only slight improvement is obtained in prediction of the two-phase region more important, however, prediction of solute distribution is improved. Incorporation of the single ternary tie line into the method of data reduction produces only a small loss of accuracy in the representation of VLE for the two binary systems. [Pg.69]

A stationary ensemble density distribution is constrained to be a functional of the constants of motion (globally conserved quantities). In particular, a simple choice is pip, q) = p (W (p, q)), where p (W) is some fiinctional (fiinction of a fiinction) of W. Any such fiinctional has a vanishing Poisson bracket (or a connnutator) with Wand is thus a stationary distribution. Its dependence on (p, q) through Hip, q) = E is expected to be reasonably smooth. Quanttun mechanically, p (W) is die density operator which has some fiinctional dependence on the Hamiltonian Wdepending on the ensemble. It is also nonnalized Trp = 1. The density matrix is the matrix representation of the density operator in some chosen representation of a complete orthononnal set of states. If the complete orthononnal set of eigenstates of die Hamiltonian is known ... [Pg.385]

The wave paeket motion of the CH eliromophore is represented by simultaneous snapshots of two-dimensional representations of the time-dependent probability density distribution... [Pg.1074]

Figure Bl.2.7. Time domain and frequency domain representations of several interferograms. (a) Single frequency, (b) two frequencies, one of which is 1.2 times greater than the other, (c) same as (b), except the high frequency component has only half the amplitude and (d) Gaussian distribution of frequencies. Figure Bl.2.7. Time domain and frequency domain representations of several interferograms. (a) Single frequency, (b) two frequencies, one of which is 1.2 times greater than the other, (c) same as (b), except the high frequency component has only half the amplitude and (d) Gaussian distribution of frequencies.
A number of procedures have been proposed to map a wave function onto a function that has the form of a phase-space distribution. Of these, the oldest and best known is the Wigner function [137,138]. (See [139] for an exposition using Louiville space.) For a review of this, and other distributions, see [140]. The quantum mechanical density matrix is a matrix representation of the density operator... [Pg.270]

Figure 8-10. C raphical representation of/dcciu) versus u for (-t-)-3 and (-)-3 sampled at 75 evenly distributed points between -0.03 A and + 0.03 e A b Hydrogen atoins not bonded to chiral carbon atoms were not considered. Figure 8-10. C raphical representation of/dcciu) versus u for (-t-)-3 and (-)-3 sampled at 75 evenly distributed points between -0.03 A and + 0.03 e A b Hydrogen atoins not bonded to chiral carbon atoms were not considered.
Despite th ese reservation s. Mu Ilikeri population -derived atomic charges arc easy to compute. Empirical investigation shows that they have various uses, they provide approximate representation of the 3D charge distribution within a molecule. [Pg.138]

The relation between the dusty gas model and the physical structure of a real porous medium is rather obscure. Since the dusty gas model does not even contain any explicit representation of the void fraction, it certainly cannot be adjusted to reflect features of the pore size distributions of different porous media. For example, porous catalysts often show a strongly bimodal pore size distribution, and their flux relations might be expected to reflect this, but the dusty gas model can respond only to changes in the... [Pg.24]

Figure 6.10 Schematic representation of the distribution of surfactant in an emulsion polymerization. Note the relative sizes of suspended particles. [From J. W. Vanderhoff, E. B. Bradford, H. L. Tarkowski, J. B. Shaffer, and R. M. Wiley,Chem. 34 32(1962).]... Figure 6.10 Schematic representation of the distribution of surfactant in an emulsion polymerization. Note the relative sizes of suspended particles. [From J. W. Vanderhoff, E. B. Bradford, H. L. Tarkowski, J. B. Shaffer, and R. M. Wiley,Chem. 34 32(1962).]...
Fig. 2. Schematic representation of the orientational distribution function f 6) for three classes of condensed media that are composed of elongated molecules A, soHd phase, where /(0) is highly peaked about an angle (here, 0 = 0°) which is restricted by the lattice B, isotropic fluid, where aU. orientations are equally probable and C, Hquid crystal, where orientational order of the soHd has not melted completely. Fig. 2. Schematic representation of the orientational distribution function f 6) for three classes of condensed media that are composed of elongated molecules A, soHd phase, where /(0) is highly peaked about an angle (here, 0 = 0°) which is restricted by the lattice B, isotropic fluid, where aU. orientations are equally probable and C, Hquid crystal, where orientational order of the soHd has not melted completely.
The larger the value of n, the more uniform is the size distribution. Other types of distribution functions can be found in Reference 1. Distribution functions based on two parameters sometimes do not accurately match the actual distributions. In these cases a high order polynomial fit, using multiple parameters, must be considered to obtain a better representation of the raw data. [Pg.331]

Fig. 8. Representation of the current distribution in porous electrodes showing the effect of conductivities of the electrolyte and electrodes where for (a)... Fig. 8. Representation of the current distribution in porous electrodes showing the effect of conductivities of the electrolyte and electrodes where for (a)...
The dominant crystal size, is most often used as a representation of the product size, because it represents the size about which most of the mass in the distribution is clustered. If the mass density function defined in equation 33 is plotted for a set of hypothetical data as shown in Figure 10, it would typically be observed to have a maximum at the dominant crystal size. In other words, the dominant crystal size is that characteristic crystal dimension at which drajdL = 0. Also shown in Figure 10 is the theoretical result obtained when the mass density is determined for a perfectiy mixed, continuous crystallizer within which invariant crystal growth occurs. That is, mass density is found for such systems to foUow a relationship of the form m = aL exp —bL where a and b are system-dependent parameters. [Pg.348]

The principle of the measurement is described with the help of Fig. 2-7 [50]. Potential measurement is not appropriate in pipelines due to defective connections or too distant connections and low accuracy. Measurements of potential difference are more effective. Figure 3-24 contains information on the details in the neighborhood of a local anode the positions of the cathodes and reference electrodes (Fig. 3-24a), a schematic representation of the potential variation (Fig. 3-24b), and the derived values (Fig. 3-24c). Figure 2-8 should be referred to in case of possible difficulties in interpreting the potential distribution and sign. The electrical potentials of the pipeline and the reference electrodes are designated by... [Pg.124]

We need a mathematical representation of our prior knowledge and a likelihood function to establish a model for any system to be analyzed. The calculation of the posterior distribution can be perfonned analytically in some cases or by simulation, which I... [Pg.322]


See other pages where Representation of Distribution is mentioned: [Pg.127]    [Pg.219]    [Pg.59]    [Pg.430]    [Pg.580]    [Pg.35]    [Pg.2878]    [Pg.127]    [Pg.219]    [Pg.59]    [Pg.430]    [Pg.580]    [Pg.35]    [Pg.2878]    [Pg.115]    [Pg.2644]    [Pg.2709]    [Pg.310]    [Pg.123]    [Pg.141]    [Pg.416]    [Pg.497]    [Pg.35]    [Pg.161]    [Pg.164]    [Pg.116]    [Pg.453]    [Pg.1836]    [Pg.2085]    [Pg.2086]    [Pg.139]   


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Representation of the Distribution Functions

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Two-dimensional representations of the electron density distribution

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