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Scattering relationships

The scattering relationships for splnodal decomposition are more subtle. Following Cahn [ ], Nlshi, et al. [ ] described the rate of growth of the amplitude of the phase domains, R(B), as a function of the wave number, 8, as... [Pg.284]

This is the generalized three-dimensional scattering relationship for the response just above the surface at x to an oscillatory pressure just above the surface at x, due to Rayleigh wave excitation, in the case where the y component of the wavevector is constant. The three-dimensional scattering function can now be calculated. [Pg.268]

We can build a network of tube sections as shown in Figure C.3. The filter structure shown below which implements the chain of scattering relationships at the tube junctions is called a ladder filter. This is the basis of many models of the human voice. The reflection filters at each end represent the acoustic activity at the glottis (vocal folds) and at the lips. [Pg.231]

Fig. 2 shows the response of a C2 film system on a step wedge (wall thickness range 2. .. 18 mm) exposed with a X-ray tube at 160 kV. For the exposure withy-rays (Irl92 or Co60) corresponding linear relationships are obtained. From this linear relationship it is followed, that the influence of the scattered radiation and the energy dependence of the absorption coefficient can be considered by an effective absorption coefficientPcff in equation (1). [Pg.562]

Note that this relationship is in conPadiction to the well known equation for the calculation of the thickness resolving power given by Halmshaw in 111. The relationship in 111 requires explicit knowledge about built-up factors for scatter correction and the film contrast factory (depending on D) and is only valid for very small wall thickness changes compared to the nominal wall thickness. [Pg.563]

This is the basic equation for monodisperse particles in light scattering experiments. We can derive tln-ee relationships by extrapolation. [Pg.1393]

Figure Bl.9.8. Schematic diagram of the relationship between a particle distribution and the measured experimental scattering data. This figure is duplicated from [14],with pennission from Academic Press. Figure Bl.9.8. Schematic diagram of the relationship between a particle distribution and the measured experimental scattering data. This figure is duplicated from [14],with pennission from Academic Press.
As we will discuss in the next section, the scattered intensity I q) at very large q values will be proportional to the q tenn. This is the well known Porod approximation, which has the relationship... [Pg.1403]

Let us consider die scattered intensity from a binary incompressible mixture of two species (containing molecules of particle 1 and molecules of particle 2) as in (B 1.9.112) we can rewrite the relationship as... [Pg.1412]

Spectral features and their corresponding molecular descriptors are then applied to mathematical techniques of multivariate data analysis, such as principal component analysis (PCA) for exploratory data analysis or multivariate classification for the development of spectral classifiers [84-87]. Principal component analysis results in a scatter plot that exhibits spectra-structure relationships by clustering similarities in spectral and/or structural features [88, 89]. [Pg.534]

When we draw a scatter plot of all X versus Y data, we see that some sort of shape can be described by the data points. From the scatter plot we can take a basic guess as to which type of curve will best describe the X—Y relationship. To aid in the decision process, it is helpful to obtain scatter plots of transformed variables. For example, if a scatter plot of log Y versus X shows a linear relationship, the equation has the form of number 6 above, while if log Y versus log X shows a linear relationship, the equation has the form of number 7. To facilitate this we frequently employ special graph paper for which one or both scales are calibrated logarithmically. These are referred to as semilog or log-log graph paper, respectively. [Pg.207]

The relationship between transmittance and the concentration of the scattering particles is similar to that given by Beer s law... [Pg.443]

Determining Concentration by Nephelometry In nephelometry, the relationship between the intensity of scattered radiation, hy and the concentration (% w/v) of scattering particles is given as... [Pg.443]

Figure 10.1 Relationships between Iq, Ij, and The light scattered per unit volume i is also shown. Figure 10.1 Relationships between Iq, Ij, and The light scattered per unit volume i is also shown.
In developing these ideas quantitatively, we shall derive expressions for the light scattered by a volume element in the scattering medium. The symbol i is used to represent this quantity its physical significance is also shown in Fig. 10.1. [Our problem with notation in this chapter is too many i s ] Before actually deriving this, let us examine the relationship between i and 1 or, more exactly, between I /Iq and IJIq. [Pg.663]

As our discussion of scattering proceeds, we shall examine the coupling between the oscillating electrical field of light and the electrons of the scatterer in detail. First, it is useful to consider the interaction of an electric field with matter, as this manifests itself in the dielectric behavior of a substance. This will not only introduce us to the field-matter interaction, but will also provide some relationships which will be useful later. [Pg.666]

An important historic application of this relationship was the determination of Avogadro s number from measurements of light scattered by the atmosphere (see Problem 3). [Pg.678]

The seventh tool is the scatter or correlation diagram also known as an XY plot (50). This plot of one variable vs another is most useful in confirming interrelationships. Thus, scatter diagrams can verify the relationships shown in the cause and effect diagram. [Pg.371]

Fig. 6. Schematic illustration of the relationships of the original y-ray and the scattered radiations for Compton scattering where E is the energy of the incident photon, E is the energy of the recoiling electron, and E is the energy of the scattered photon. Fig. 6. Schematic illustration of the relationships of the original y-ray and the scattered radiations for Compton scattering where E is the energy of the incident photon, E is the energy of the recoiling electron, and E is the energy of the scattered photon.

See other pages where Scattering relationships is mentioned: [Pg.677]    [Pg.152]    [Pg.151]    [Pg.282]    [Pg.372]    [Pg.539]    [Pg.677]    [Pg.152]    [Pg.151]    [Pg.282]    [Pg.372]    [Pg.539]    [Pg.326]    [Pg.564]    [Pg.725]    [Pg.1391]    [Pg.1806]    [Pg.1809]    [Pg.2651]    [Pg.2882]    [Pg.2937]    [Pg.442]    [Pg.443]    [Pg.614]    [Pg.675]    [Pg.676]    [Pg.693]    [Pg.706]    [Pg.279]    [Pg.60]    [Pg.433]    [Pg.480]   
See also in sourсe #XX -- [ Pg.284 , Pg.288 ]




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