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Characteristic lines three-dimensional

Time-dependent analytical measurements, which give three-dimensional information of the type y = f(zy t) as shown schematically in Fig. 3.11a. The same characteristic holds for distribution analysis in one spatial direction, i.e., line scans, y = f(zylx). Such signal functions are frequently represented in form of multiple diagrams as shown in Fig. 3.11b. [Pg.81]

ESP and electron density maps were obtained by analytical calculations using the program MOLPROP with parameters for the K-model Characteristic peculiarities in the ESP along bonding lines are seen in the (110) map for MgO (Fig. 6). All peculiarities in the ESP distribution can be seen, i.e. in the form of maximums on the nuclei and at one-, two-, and three-dimensional minimums in the inter-nuclear areas. [Pg.111]

Fig. 2.8 Cleavage in the amphiboles. (A) Schematic representation of the characteristic stacked amphibole I-beams in the three-dimensional structure. A tetrahedral portion of an I-beam is labeled "silica ribbon." The octahedral portion is labeled "cation layer" and represented by solid circles. One of the possible cleavage directions (110) along planes of structural weakness is indicated by the line A-A stepped around the I-beams in the lower part of the diagram. (B) Cross section of the stacked I-beams with the directions of easy cleavage indicated. There is a lower density of bonds between I-beams in the crystallographic directions (110) and (110). These directions, parallel to the c axis and the length of the chains, are the planes of cleavage. The minimum thickness of a rhombic fragment produced through cleavage is 0.84 nm. Fig. 2.8 Cleavage in the amphiboles. (A) Schematic representation of the characteristic stacked amphibole I-beams in the three-dimensional structure. A tetrahedral portion of an I-beam is labeled "silica ribbon." The octahedral portion is labeled "cation layer" and represented by solid circles. One of the possible cleavage directions (110) along planes of structural weakness is indicated by the line A-A stepped around the I-beams in the lower part of the diagram. (B) Cross section of the stacked I-beams with the directions of easy cleavage indicated. There is a lower density of bonds between I-beams in the crystallographic directions (110) and (110). These directions, parallel to the c axis and the length of the chains, are the planes of cleavage. The minimum thickness of a rhombic fragment produced through cleavage is 0.84 nm.
A more complicated situation emerges in motion along nonintersecting surfaces with variable curvatures. If the distance between these surfaces remains finite everywhere, then the field lines do not expand infinitely in the directions normal to the surfaces. In the absence of dissipation this means that there is no unbounded growth of the normal field component. However, introduction of the finite conductivity yields an equation for the normal component which is not decoupled it contains the contribution of the Laplacian of the remaining components. At the same time, it is possible for all other components to increase exponentially with an increment which depends on the conductivity and vanishes for infinite conductivity. The authors called this mechanism of field amplification a slow dynamo, in contrast to the fast dynamo feasible in the three-dimensional case, i.e., the mechanism related only to infinite expansion of the field lines as, for example, in motion with magnetic field loop doubling. In a fast dynamo the characteristic time of the field increase must be of the same order as the characteristic period of the motion s fundamental scale. [Pg.105]

A characteristic feature of these partially oxidized bis(oxalato)platinate salts of divalent cations is the coexistence of two modulations of the lattice over a wide temperature range (a) a one-dimensional modulation, as detected by the appearance of diffuse lines on X-ray films, perpendicular to the [Pt(C204)2] anion stacking direction and surrounding the even Bragg reflection layer lines of non-zero order (b) a three-dimensional modulation which gives rise to a complicated pattern of fine satellite spots in the neighbourhood of every reciprocal layer line. [Pg.141]

Students will identify different characteristics of line as seen in example reproductions of professional two- and three-dimensional artwork and in the film. [Pg.228]

The cervical section presented in Fig. 10.7 has been diagnosed as a rare form of neoplasma known as villoglandular adenocarcinoma. Characteristic cytologic features of this condition include the presence of long villous fronds and papillae lined by columnar cells with intact cytoplasmic borders and minimal atypia.32 Three-dimensional ball-like clusters of cells with smooth intact communal cytoplasmic rings are also associated with this condition.32... [Pg.222]

The three-dimensional structure of human extracellular superoxide dismutase (EC-SOD) is unknown. Studies of structure-function relationships have been severely limited by its poor production in mammalian cell lines and failure to be expressed in prokaryotic and yeast systems. In contrast, extra- and intracellular Cu- and Zn-containing superoxide dismutases (CuZn-SOD) are expressed very well in E. coli and yeast. CuZn-SOD is homologous to a large interior fragment of EC-SOD, but lacks its extra N-terminal and C-terminal domains. Fusions of either the N-terminal domain of EC-SOD or both the N- and C-terminal domains of EC-SOD to CuZn-SOD resulted in a domain-swapped enzyme that expressed well and whose characteristics resemble EC-SOD (Stenlund and Tibell, 1999). [Pg.46]

Because of the complexity of Fig. 12.1, the detailed characteristics of binary VLB are usually depicted by two-dimensional graphs that display what is seen on various planes that cut the three-dimensional diagram. The three principal planes, each perpendicular to one of the coordinate axes, are illustrated in Fig. 12.1. Thus a vertical plane perpendicular to the temperature axis is outlined as ALBDEA. The lines on this plane represent a Pxy phase diagram at constant T, of which we have already seen examples in Figs. 10.1, 11.7, 11.9, and 11.11. If the lines from several such planes are projected on a single parallel plane, a diagram like Fig. 12.2 is obtained. It shows Pxy plots for three different temperatures. The one for represents the section of Fig. 12.1 indicated by ALBDEA. [Pg.581]

For example, in a six component system, three equal characteristic roots means that all reaction paths will be straight lines in a particular three dimensional subspace of the five dimensional simplex. [Pg.232]

A fundamental characteristic of a fractal is its fractal dimension. Suppose we draw a sphere of radius r around a point in the object. If the fractal object is a line, the mass M(r) within the sphere will be proportional to r. If it is a sheet, then M(r) oc r2. If it is a solid three-dimensional object, M r) would be proportional to r3. In a fractal, the following general relation is obeyed,... [Pg.189]


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See also in sourсe #XX -- [ Pg.113 ]

See also in sourсe #XX -- [ Pg.113 ]




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Characteristics dimensionality

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