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Wave ring

Figure12.11 Sealing systems (a) O-ring atthe face (b) O-ring inside the bore (c) double O-ring carrier (d) metallic wave ring. Figure12.11 Sealing systems (a) O-ring atthe face (b) O-ring inside the bore (c) double O-ring carrier (d) metallic wave ring.
Figure C3.6.8 (a) A growing ring of excitation in an excitable FitzHugh-Nagumo medium, (b) A spiral wave in tlie same system. Figure C3.6.8 (a) A growing ring of excitation in an excitable FitzHugh-Nagumo medium, (b) A spiral wave in tlie same system.
The furanose rings of the deoxyribose units of DNA are conformationally labile. All flexible forms of cyclopentane and related rings are of nearly constant strain and pseudorotations take place by a fast wave-like motion around the ring The flexibility of the furanose rings (M, Levitt, 1978) is presumably responsible for the partial unraveling of the DNA double helix in biological processes. [Pg.344]

The preparation of 5-azothiazoles uses the nucleophilic character of C-5 carbon in reaction with the appropriate diazonium salt (402, 586). These 5-azothia2oles form 1 1 complexes with Ag (587). 2-Amino-4-methyl-5-arylazothiazoles give reduction waves involving two-electron transfer the Ej/ values correlate to the angle between the thiazole and phenyl rings (588). [Pg.108]

For Woodward-Hoffman allowed thermal reactions (such as the conrotatory ring opening of cyclobutane), orbital symmetry is conserved and there is no change in orbital occupancy. Even though bonds are made and broken, you can use the RHF wave function. [Pg.46]

Fig. 10. The rotary actuator (a) side view where SAW = surface acoustic wave and (b) view of the poled pie2oelectric ceramic ring showing poled segments and how temporal and spatial phase differences are estabUshed. Courtesy of Shinsei Kogyo Co. Fig. 10. The rotary actuator (a) side view where SAW = surface acoustic wave and (b) view of the poled pie2oelectric ceramic ring showing poled segments and how temporal and spatial phase differences are estabUshed. Courtesy of Shinsei Kogyo Co.
Transmission electron microscopy (tern) is used to analyze the stmcture of crystals, such as distinguishing between amorphous siUcon dioxide and crystalline quartz. The technique is based on the phenomenon that crystalline materials are ordered arrays that scatter waves coherently. A crystalline material diffracts a beam in such a way that discrete spots can be detected on a photographic plate, whereas an amorphous substrate produces diffuse rings. Tern is also used in an imaging mode to produce images of substrate grain stmctures. Tern requires samples that are very thin (10—50 nm) sections, and is a destmctive as well as time-consuming method of analysis. [Pg.356]

The reverse reaction, the photochemical ring opening of sphopyranes (22b), takes place by absorption ia the short-wave uv region of the spectmm and the merocyanine isomer (22a) is obtained. The electron transition of (22a) is ia the visible spectral region, whereas (22b) is colorless. As a result, the dye solution can change from colorless to a colored solution (87,88). These photochromic reactions can be used for technical appHcations (89). [Pg.496]

Semiconductor materials are rather unique and exceptional substances (see Semiconductors). The entire semiconductor crystal is one giant covalent molecule. In benzene molecules, the electron wave functions that describe probabiUty density ate spread over the six ting-carbon atoms in a large dye molecule, an electron might be delocalized over a series of rings, but in semiconductors, the electron wave-functions are delocalized, in principle, over an entire macroscopic crystal. Because of the size of these wave functions, no single atom can have much effect on the electron energies, ie, the electronic excitations in semiconductors are delocalized. [Pg.115]

Fig. 6.6. One-dimensional, pressure-versus-location predictions at various times are shown for a typical powder compact subjected to baratol plane-wave explosive loading. The pressure is shown to ring-up to a final value between the copper end plates (after Graham [87G03]). Fig. 6.6. One-dimensional, pressure-versus-location predictions at various times are shown for a typical powder compact subjected to baratol plane-wave explosive loading. The pressure is shown to ring-up to a final value between the copper end plates (after Graham [87G03]).

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