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Bending umbrella

Chain CH2 sci + rock 773.5 Chain CH2 rock + ring C-H oopl iph bend (umbrella)... [Pg.323]

In addition to the descriptions of group vibrations as stretch and bend (or deformation) the terms rock, twist, scissors, wag, torsion, ring breathing and inversion (or umbrella) are used frequently these motions are illustrated in Figure 6.13. [Pg.157]

In addition, X-ray diffraction analysis of related molecules reveals that in the sixth (formally unoccupied) position of the octahedron the metallic center is well shielded. Four of the 12 methyl groups of the phosphine ligands surround the metal like an umbrella. As a result of the shielding effect of the methyl groups, a bending of the phosphorus-metal-phosphorus axis is observed.24... [Pg.5]

Figure 3.23 Bond bending in umbrella inversion vibration of NH3 (circles, solid line) and PH3 (squares, dotted line), comparing the lp—A—H umbrella angle for nuclei (0nuciei) and hybrids ( nho)- An inscribed triangle marks the equilibrium geometry for each molecule, and the dashed line marks the limit of perfect orbital... Figure 3.23 Bond bending in umbrella inversion vibration of NH3 (circles, solid line) and PH3 (squares, dotted line), comparing the lp—A—H umbrella angle for nuclei (0nuciei) and hybrids ( nho)- An inscribed triangle marks the equilibrium geometry for each molecule, and the dashed line marks the limit of perfect orbital...
Fixed-Roof Tanks. The effect of internal pressure on plate structures, including tanks and pressure vessels, is important to tank design. If a flat plate is subjected to pressure on one side, it must be made quite thick to resist bending or deformation. A shallow cone-roof deck on a tank approximates a flat surface and is typically built of 3/ 16-in. (4.76-mm) thick steel (Fig. 4a). This is unable to withstand more than a few inches of water column pressure. The larger the tank, the more severe the effect of pressure on the structure. As pressure increases, the practicality of fabrication practice and costs force the tank builder to use shapes more suitable for internal pressure. The cylinder is an economic and easily fabricated shape for pressure containment. Indeed, almost all large tanks are cylindrical. The problem, however, is that the ends must be closed. The relatively flat roofs and bottoms or closures of tanks do not lend themselves to much internal pressure. As internal pressure increases, tank builders use roof domes or spheres. The spherical tank is the most economic shape for internal pressure storage in terms of required thickness, but it is generally more difficult to fabricate than a dome- or umbrella-roof tank because of its compound curvature. [Pg.311]

There has been a flurry of recent activity in the study of the photodissociation dynamics of this molecule (186,187,188). Hermann and Leone used the infrared luminescence technique with a circular variable filter to determine the IR emission as a function of frequency when this molecule was photolyzed with lasers at 248 and 266 nm. From their results, they were able to show that the umbrella bending V2 mode of the CH3 radical was the only mode of CH3 that was excited in the photofragmentation of CH3I. This is in accord with the idea that the photodissociation of this molecule is unusually simple, and involves primarily the scission of the C-I bond with the simultaneous relaxation of the pyramidal structure of the CH3 part of the molecule into its final planar form. The data are used to obtain a vibrational distribution of the CH3 radical that peaks at v" = 2 and extends all the way out to the v" = 10 level. [Pg.66]

The edge of the cap of this species generally undulates, resembling a bottle cap or lawn umbrella, and the stem is often characterized by twisting bends. An important identifying characteristic is a brown spot that appears in the center of the cap after it is dried. Psilocybe baeocystis is bound to become more familiar because of increasingly widespread use of its host materials in industrial parks, around homes, etc. [Pg.353]

Figure 13. Comparison of the best fit experimental thermal rate coefficient with the total value for the JG PES. the ab initio PES. and the contribution from the initial CH stretch (nOO). HCH bend (OnO), and umbrella (OOn) states. Figure 13. Comparison of the best fit experimental thermal rate coefficient with the total value for the JG PES. the ab initio PES. and the contribution from the initial CH stretch (nOO). HCH bend (OnO), and umbrella (OOn) states.
Certain particular failures should be noted. The frequency of the out-ofplane symmetric vibration of CH3 was found to be too low for all the DFT methods. The same is also true for the three ab initio methods. For the umbrella motion of NH3, too high a value is found by all methods. For the symmetric bending vibration of C2H2, all of the theoretical values except HF are too low. [Pg.207]

Also, our normal coordinate analysis revealed that the Cr-CO-, ring-Cr-C-and the C-Cr-C-bending coordinates are strongly coupled in E symmetry. In AI symmetry, the C-Cr-C umbrella opening mode is coupled with the Cr-C-O parallel bend. For details of the assignments the reader is referred to Table 12, in which we also included mode descriptions based on the criterion of potential energy distribution. The frequency related to the B2U C-C stretching vibration is overestimated, as it is for free benzene and for BzaCr. [Pg.68]


See other pages where Bending umbrella is mentioned: [Pg.95]    [Pg.40]    [Pg.95]    [Pg.40]    [Pg.149]    [Pg.8]    [Pg.343]    [Pg.215]    [Pg.342]    [Pg.275]    [Pg.259]    [Pg.100]    [Pg.233]    [Pg.234]    [Pg.99]    [Pg.275]    [Pg.250]    [Pg.565]    [Pg.567]    [Pg.568]    [Pg.568]    [Pg.253]    [Pg.255]    [Pg.256]    [Pg.276]    [Pg.280]    [Pg.239]    [Pg.23]    [Pg.129]    [Pg.253]    [Pg.255]    [Pg.256]    [Pg.276]    [Pg.280]    [Pg.131]    [Pg.250]    [Pg.1583]    [Pg.323]    [Pg.58]    [Pg.97]   
See also in sourсe #XX -- [ Pg.5 ]




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