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Structure isometric

For the triiodides, more generally, we might also choose to remove the restriction of colinearity of the three atoms, in which case there are no outer atoms and no inner one. We would then need to specify three interatomic distances to describe the molecules say d, c 3i of lengths a, b, and c, respectively. There are now six permutations, i.e. six ways of choosing the atomic labels or the corresponding interatomic distances that lead to isometric structures. [Pg.24]

Analogous considerations apply to interconversions of MX5 molecules between trigonal bipyramidal structures via, for example, square pyramidal ones, or to interconversions of MXg molecules between octahedral structures via trigonal prismatic ones (see Chapter 8), and, quite generally, to all interconversion processes between isometric structures. A more rigorous treatment of these problems would have to take into account the concept of the permutation-inversion group [23]. [Pg.49]

In these examples, isometric structures are interconnected by large distortions that trace possible interconversion pathways between alternative reference structures. Instead of defining configuration space relative to a single symmetric reference structure it is advantageous in these cases to have a symmetrical description of the relevant portion of configuration space and thereby of the entirety of geometric transformations between isometric structures. [Pg.49]

Fig. 2.10. Isometric structures of the ethane molecule, obtained by symmetry operations of the point group Dj and by rotation of one methyl group with respect to the other... Fig. 2.10. Isometric structures of the ethane molecule, obtained by symmetry operations of the point group Dj and by rotation of one methyl group with respect to the other...
We now enumerate the ways in which this arbitrary conformation can be converted into an isometric structure. First, the enantiomorphic conformation can be obtained by reversing the signs of the torsion angles (pi- — 02- Second, because... [Pg.52]

In this chapter we have discussed symmetry aspects of molecular structure, with emphasis on the symmetry of small distortions from a symmetric reference structure and on the interconversions between isometric structures, which mostly involve large distortions. In the language of configuration space, such interconversions take the form of pathways between equivalent points. In Sections 2.4.3, 2.6.1 and 2.6.3-5 we have described specific examples of such pathways and related them to the molecular potential energy surface. A more detailed discussion of the use of symmetry arguments in deriving properties of the energy surface is included in Chapter 5. [Pg.68]

The compliance in series with the active force. Force exerted by the activated elements must be transmitted or borne by whatever structural elements are in series with them. In skeletal muscle there is clearly a tendon in series but not so with smooth muscle. In smooth muscle, the total length of contractile apparatus is broken up into individual cells with intercalating extracellular connective structures. In addition, the portions of the crossbridges in series with the pulling site must also be stretched before force can rise to isometric levels. Taken together, the... [Pg.167]

In each of the composition diagrams in Fig. 14.2, the numbers represent a series of reactions run at a defined composition and temperature. These are isometric sulfur slices through three-dimensional K/P/RE/S quaternary phase diagrams. As just one example of what we have studied. Table 14.1 identifies the compositions at each point and the resulting phase(s). We have rigorously studied how phase formation is dependent upon the compositions of reactions for the rare-earth elements Y, Eu, and La and we have also discovered key structural relationships between the rare-earth elements, indicating a significant dependence on rare-earth and alkali-metal size for sulfides and selenides. [Pg.211]

Figure 69 shows the solid-state structure of the thermodynamically more stable homochiral dimer (7 , )-145,210 which features a highly puckered central (Zn-0)2 ring with almost isometric Zn-O bond lengths. [Pg.373]

The solid-state structure of 166 shows that the pentamethylcyclopentadienyl ligands are symmetrically bound to the zinc atoms in a pentahapto fashion, with isometric Zn-C bonds, ranging from 2.27 to 2.30 A. [Pg.381]

Twenty five years on from the first spherical virus structures, the complexity of the isometric virus... [Pg.245]

Although the correlation between ionic porosity and diffusivity is imperfect, there is a rough trend that oxygen diffusivity in the minerals increases with increasing IP. The trend is useful in qualitative estimation of closure temperature (among other applications). Extending the relation to metallic systems, one prediction is that diffusion in face-centered cubic structure (25.95% free space) is slower that that in body-centered structure (31.98% free space) of the same metal composition. To avoid the issue of anisotropy, it would be worthwhile to reexamine the relations between diffusivity and ionic porosity using only isometric minerals. [Pg.311]

Chromium(III) oxide crystallizes in the rhombohedral structure of the corundum type space group D3d-R3c, Q 5.2 g/cm3. Because of its high hardness (ca. 9 on the Mohs scale) the abrasive properties of the pigment must be taken into account in certain applications [3.44], It melts at 2435 °C but starts to evaporate at 2000 °C. Depending on the manufacturing conditions, the particle sizes of chromium oxide pigments are in the range 0.1-3 pm with mean values of 0.3-0.6 pm. Most of the particles are isometric. Coarser chromium oxides are produced for special applications, e.g., for applications in the refractory area. [Pg.94]

Fig. 6.1.6. Block structure of shiny smooth faces (001), (Oil), (110), (111) 0f sulphur isometric crystal shown by hardness testing. Fig. 6.1.6. Block structure of shiny smooth faces (001), (Oil), (110), (111) 0f sulphur isometric crystal shown by hardness testing.
Argentite is probably die most important primary silver mineral. However, it maintains its cubic (isometric) characteristic only above 179 C (354°F). Upon cooling, the inward structure inverts to a noil-isometric form, usually orthorhombic, yet retaining its original outward form. It is, therefore, a paramorph after argentite, known as acanthite. [Pg.146]

The maximum number of isometric re-structures NC (Xk( e), Zk equals l ( )l. This set of restructures decomposes for each particular isotopic modification NC Xk(f ), Zk, Mk into subsets of isomers (nonisometric NCs). Each isomer is associated with a coset of the decomposition of W ( ) modulo ( ) (e = I ( ) I, ... [Pg.75]


See other pages where Structure isometric is mentioned: [Pg.15]    [Pg.23]    [Pg.36]    [Pg.50]    [Pg.51]    [Pg.54]    [Pg.213]    [Pg.77]    [Pg.842]    [Pg.578]    [Pg.1341]    [Pg.15]    [Pg.23]    [Pg.36]    [Pg.50]    [Pg.51]    [Pg.54]    [Pg.213]    [Pg.77]    [Pg.842]    [Pg.578]    [Pg.1341]    [Pg.271]    [Pg.967]    [Pg.359]    [Pg.366]    [Pg.493]    [Pg.245]    [Pg.246]    [Pg.482]    [Pg.135]    [Pg.116]    [Pg.217]    [Pg.83]    [Pg.76]    [Pg.752]    [Pg.1008]    [Pg.46]    [Pg.26]    [Pg.70]   
See also in sourсe #XX -- [ Pg.38 ]




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