Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Position circles

Vibrating grizzlies. These are simply bar grizzlies mounted on eccentrics so that the entire assembly is given a back-and-forth movement or a positive circle throw. These are made by companies such as AUis-Chalmers, Hewitt Robins, Nordberg, Link-Belt, Simphcity, and Tyler. [Pg.1772]

Figure 21. Energy-migration patterns in tetranuclear compounds. Empty and full labels indicate and Os, respectively. In the peripheral positions, circles and squares indicate M(bpy)j and M(biq)j components, respectively. For the bridging ligands -W- = 2,3-dpp — 2,5-dpp. Figure 21. Energy-migration patterns in tetranuclear compounds. Empty and full labels indicate and Os, respectively. In the peripheral positions, circles and squares indicate M(bpy)j and M(biq)j components, respectively. For the bridging ligands -W- = 2,3-dpp — 2,5-dpp.
Fig. 23a. Stress-strain-diagram of a Polyethylene (Vestolen A 6042) film (stretching velocity 0,26 mm/s) b) Experimental (row I), synthesized (row II), and resolved (row III) bands of the CHj-rocking bands. The experimental spectra were scanned at the indicated positions (circled numbers) of the stress-strain-diagram (a). Fig. 23a. Stress-strain-diagram of a Polyethylene (Vestolen A 6042) film (stretching velocity 0,26 mm/s) b) Experimental (row I), synthesized (row II), and resolved (row III) bands of the CHj-rocking bands. The experimental spectra were scanned at the indicated positions (circled numbers) of the stress-strain-diagram (a).
Fig. 16. STM images of the same area of a PtCo(l 11) surface alloy showing (a) chemical contrast (Pt atoms appear bright) and (b) the adsorbed CO molecules at saturation coverage. Frame (c) shows a schematic view of the CO positions (circles) on the alloy atoms (small black and grey squares for Co and Pt, respectively) in the lower right quadrant of frames (a) and (b). Frame (d) shows the probability of finding a CO molecule on a given Pt atom as a function of the number of its Co neighbours in the first layer for low CO coverage (0.1 L) and saturation coverage [66]. Fig. 16. STM images of the same area of a PtCo(l 11) surface alloy showing (a) chemical contrast (Pt atoms appear bright) and (b) the adsorbed CO molecules at saturation coverage. Frame (c) shows a schematic view of the CO positions (circles) on the alloy atoms (small black and grey squares for Co and Pt, respectively) in the lower right quadrant of frames (a) and (b). Frame (d) shows the probability of finding a CO molecule on a given Pt atom as a function of the number of its Co neighbours in the first layer for low CO coverage (0.1 L) and saturation coverage [66].
Fig. 15.6. Schematic representation of a sequence of a stretched polystyrene chain. The succession of points displays the carbon skeleton. The hexagons represent benzene rings. Two consecutive rings lying on the same side of the skeleton are in isotactic position. Circles o represent hydrogens bound to the skeleton. Fig. 15.6. Schematic representation of a sequence of a stretched polystyrene chain. The succession of points displays the carbon skeleton. The hexagons represent benzene rings. Two consecutive rings lying on the same side of the skeleton are in isotactic position. Circles o represent hydrogens bound to the skeleton.
A.3 WHERE IS Zi LOCATED ON THE TRANSFORMATION CIRCLE DETERMINATION OF THE POSITION CIRCLES... [Pg.286]

The position circles are obtained completely analogous to the impedance case in row 1. [Pg.293]

A.3 Where is Z Located on the Transformation Circle Determination of the Position Circles / 286... [Pg.370]

The frictional force may also depend on the direction of sliding, and the relative orientation and registry of the two walls. The situation is illustrated in Figure 1 which shows a representative contour plot of the energy as a function of position as a single monomer moves over a (111) surface. The maximum energy positions (circles)... [Pg.93]

Figure 3-15 Intermaterial area density distribution for two cases of the sine flow at T = 1.6 (almost globally chaotic). The figure compares the distribution computed from the coarse-grained stretching field to the distribution computed from direct tracking of a continuous material filament. Although the latter method cannot be applied to most chaotic flows, the first case is a fairly straightforward computation in both model and real chaotic flows. The distributions of p are shown as a function of initial position (square), as a function of final position (circles), and as computed from direct filament tracking (triangles). All three curves collapse onto a single distribution. Figure 3-15 Intermaterial area density distribution for two cases of the sine flow at T = 1.6 (almost globally chaotic). The figure compares the distribution computed from the coarse-grained stretching field to the distribution computed from direct tracking of a continuous material filament. Although the latter method cannot be applied to most chaotic flows, the first case is a fairly straightforward computation in both model and real chaotic flows. The distributions of p are shown as a function of initial position (square), as a function of final position (circles), and as computed from direct filament tracking (triangles). All three curves collapse onto a single distribution.
Fig. 67. - Planar pattern of variously positioned circles (upper), which repeated motif (left) gives the image of agglomerates of globular niacromolecules spaced in the micro-world (middle) or the macroscopically visual view of the Universe (right). Below the repetitive (ornamental) motif showing its certain resemblance with a microstructure of crystallites. Fig. 67. - Planar pattern of variously positioned circles (upper), which repeated motif (left) gives the image of agglomerates of globular niacromolecules spaced in the micro-world (middle) or the macroscopically visual view of the Universe (right). Below the repetitive (ornamental) motif showing its certain resemblance with a microstructure of crystallites.
Figure 2.24 Enlargement of small area (rectangle Figure 2.4) from 2D photoelastic disks under simple shear viewed through a dark-field circular polariscope. (a) Experiment. (Courtesy of J. Ren and R. P. Behringer, Duke University, Durham, NC.) (b) Calculated reconstruction used to extract the interparticle forces, (c) Least squares image used to determine the initial guesses for the contact points and final contact positions (circles). Figure 2.24 Enlargement of small area (rectangle Figure 2.4) from 2D photoelastic disks under simple shear viewed through a dark-field circular polariscope. (a) Experiment. (Courtesy of J. Ren and R. P. Behringer, Duke University, Durham, NC.) (b) Calculated reconstruction used to extract the interparticle forces, (c) Least squares image used to determine the initial guesses for the contact points and final contact positions (circles).

See other pages where Position circles is mentioned: [Pg.258]    [Pg.281]    [Pg.281]    [Pg.282]    [Pg.284]    [Pg.286]    [Pg.287]    [Pg.292]    [Pg.293]    [Pg.369]    [Pg.182]    [Pg.334]   
See also in sourсe #XX -- [ Pg.281 , Pg.282 , Pg.283 , Pg.284 , Pg.285 , Pg.286 , Pg.293 , Pg.294 , Pg.295 , Pg.296 ]




SEARCH



Circle

© 2024 chempedia.info