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Symmetry right/left

Structure of a-selenium. Left side view of a helix with 3j 2 screw symmetry. Right view along the helices the unit cell and the coordination about one atom are plotted... [Pg.107]

Of the two one-dimensional arrangements shown in figure 2, the disordered state has the higher symmetry since left and right directions are equivalent. [Pg.503]

Fig. 5.5. Geometrical structure of a close-packed metal surface. Left, the second-layer atoms (circles) and third-layer atoms (small dots) have little influence on the surface charge density, which is dominated by the top-layer atoms (large dots). The top layer exhibits sixfold symmetry, which is invariant with respect to the plane group p6mm (that is, point group Q, together with the translational symmetry.). Right, the corresponding surface Brillouin zone. The lowest nontrivial Fourier components of the LDOS arise from Bloch functions near the T and K points. (The symbols for plane groups are explained in Appendix E.)... Fig. 5.5. Geometrical structure of a close-packed metal surface. Left, the second-layer atoms (circles) and third-layer atoms (small dots) have little influence on the surface charge density, which is dominated by the top-layer atoms (large dots). The top layer exhibits sixfold symmetry, which is invariant with respect to the plane group p6mm (that is, point group Q, together with the translational symmetry.). Right, the corresponding surface Brillouin zone. The lowest nontrivial Fourier components of the LDOS arise from Bloch functions near the T and K points. (The symbols for plane groups are explained in Appendix E.)...
Fig. 18. Energy level diagrams for the cobalt(II) ion in a five-coordinate chromo-phore. Left, Dsn symmetry. Right, the effect of the variation of jS angle on the energy levels (Dq = 1 kK)... Fig. 18. Energy level diagrams for the cobalt(II) ion in a five-coordinate chromo-phore. Left, Dsn symmetry. Right, the effect of the variation of jS angle on the energy levels (Dq = 1 kK)...
Fig. 3. Relative energies for spin states of the [FeJ cluster 2 on optimized structures of spin symmetry given (left panel) as well as single points at the high-spin structure (right panel). The BS solution is not displayed. Fig. 3. Relative energies for spin states of the [FeJ cluster 2 on optimized structures of spin symmetry given (left panel) as well as single points at the high-spin structure (right panel). The BS solution is not displayed.
If you find yourself confused about the d,l, and meso forms of tartaric acid, a simple analogy may help keep matters straight. Consider three sets of shoes. A right shoe beside a left shoe is a meso combination with a plane of symmetry. A left shoe next to a left shoe is not identical with, but is... [Pg.137]

Scheme 2.12 Representations of the structure of human H chain ferritin viewed down the four- and three-fold symmetry axes (left and right respectively). The interactions about the fourfold axis are at 90° and are based on four subunit tetramers. Protein trimers arranged at 60 degrees to one another form the three-fold axis. (Reproduced with permission from Reference 20). Scheme 2.12 Representations of the structure of human H chain ferritin viewed down the four- and three-fold symmetry axes (left and right respectively). The interactions about the fourfold axis are at 90° and are based on four subunit tetramers. Protein trimers arranged at 60 degrees to one another form the three-fold axis. (Reproduced with permission from Reference 20).
Fig. 30. Two views of the structure of [Gd(dota)] showing the encapsulation of the metal ion by the four pendant arms (left) and the C4 symmetry (right, top view). Redrawn from (Chang et al., 1993). Fig. 30. Two views of the structure of [Gd(dota)] showing the encapsulation of the metal ion by the four pendant arms (left) and the C4 symmetry (right, top view). Redrawn from (Chang et al., 1993).
Equation (8.8), the essential result of this section, provides the general condition under which electric fields, assuming a dipole interaction, can break the right-left. symmetry of the initial state and result in enhanced production of a desired enan- tiomer. Specifically, the difference between the amount of D and L formed is seen to tiej)end entirely on the difference between the molecular dynamics when irradiated % E and by — E. Hence, we can state that a necessary condition for nonzero epahtiomeric excess, and the brealdng of the left-right symmetry, is that the... [Pg.169]

Used for planar systems in which e(z) varies continuously in the direction z perpendicular to the planar interfaces, with a variation of e in finite layer of thickness Da next to the left-hand-side space of material A (or L in Level 3), za = — z (measured leftward for symmetry in left-hand-side and right-hand-side notation). [Pg.105]

Clark (1969, 1973) and others (Lakoff Johnson, 1980 see also Tversky, this volume) maintain that this asymmetry of linguistic structure is rooted in the asymmetries of perceptual space. The clearest form of this argument was given by Clark, who pointed out that the structure of our bodies and our movements in the world define three reference planes, two of which are asymmetrical. The only plane characterized by perceptual symmetry is the right-left plane. Two reference planes are asymmetrical the front-back plane, and the top-bottom (or head-feet) plane. Clark claimed that the front end of the front-back plane is positive because it is the direction of movement and the side toward which most of our perceptual receptors are oriented. Similarly, he reasoned that the top end of the top-bottom plane is positive because up-down is the canonical orientation of the body as well as the primary direction of observed movement (objects fall from up to down but never in the opposite direction). The asymmetric structure of perceptual space has since been confirmed... [Pg.228]

Figure 8-36. Wall decorations with symmetry planes (left) and without (right) in the Alhambra, Granada, Spain (photographs by the authors). Figure 8-36. Wall decorations with symmetry planes (left) and without (right) in the Alhambra, Granada, Spain (photographs by the authors).
Symmetry also brings beauty and simplicity to physics. Symmetries are embedded in namre and the physical laws that describe the phenomena of nature have this same symmetry embedded in them. Symmetry, in turn, means that the laws of physics are invariant under the symmetry operation. For example, parity symmetry, P, implied that the same laws describe physical phenomena when right and left are interchanged. A violation of this symmetry was found that destroyed the absolute character of the right-left invariance. [Pg.233]

Fig. 6 DOR has icosahedral symmetry (left) and DAS has cubic symmetry (right)... Fig. 6 DOR has icosahedral symmetry (left) and DAS has cubic symmetry (right)...
Figure 7. Pictorial representation of the pathways in Liouville space that contribute to SRF spectra. Solid lines denote radiative coupling V. Horizontal (vertical) lines represent action of V from the right (left). The SRF process is obtained by all pathways that start at aa and end at cc in fourth order (four bonds). There are six pathways that contribute. However, owing to symmetry, we need consider only the three pathways shown in Fig. 8. The other three are obtained by a complex conjugation and permutation of b and d. Figure 7. Pictorial representation of the pathways in Liouville space that contribute to SRF spectra. Solid lines denote radiative coupling V. Horizontal (vertical) lines represent action of V from the right (left). The SRF process is obtained by all pathways that start at aa and end at cc in fourth order (four bonds). There are six pathways that contribute. However, owing to symmetry, we need consider only the three pathways shown in Fig. 8. The other three are obtained by a complex conjugation and permutation of b and d.
The starting point for the evaluation of the turnover expression for the escape rate (117) is an equation for the stationary flux of particles exiting each well at either barrier. The number of particles per unit energy and per unit time hitting the right (left) barrier of the jth well with positive (negative) velocity is denoted by // (/ ). The reflection symmetry of the potential and the boundary conditions about the zeroth well implies that... [Pg.661]

Figure 27.4. Left Si-O-Al-O-Sn skeleton in (Ph2Si0)g-(A102)4Sn2 with almost S4 symmetry. Right Polyhedral representation of Li5(Ph2Si0)i2(A102)2 [A10i. 5(0H)]4 with the lithium cations in the holes of the polycyclic structure. Figure 27.4. Left Si-O-Al-O-Sn skeleton in (Ph2Si0)g-(A102)4Sn2 with almost S4 symmetry. Right Polyhedral representation of Li5(Ph2Si0)i2(A102)2 [A10i. 5(0H)]4 with the lithium cations in the holes of the polycyclic structure.
Fig. 23. Cjv ligand field model for intrazeolite transition-metal ion complexes (left). Changes of the one-electron energy levels starting from the free ion and switching on fields of spherical, C y and symmetry (right). Reprinted from [32] with permission of Academic Press, Inc... [Pg.379]

One speaks of a violation of the symmetry (here parity violation). It should be noted that the modern R, S nomenclature is used in the figure, whereby the R-amino acids normally correspond to the D-amino acids in the old nomenclature and the 5-amino acids correspond to the L-amino acids. We shall use both nomenclatures here, because the D, L terminology is widely used in biochemistry. In physics, one tends to use the R, L nomenclature which simply stands for Right/Left. If one takes into account the chemical equilibrium (3.1) at room temperature, the small enthalpy of reaction is reflected in the equilibrium constant ... [Pg.50]

This means that the horse in its movements does not prefer its right (left) side over its left (right) side. This, does not mean that taking a picture of such a horse results in a perfect symmetry in the picture. Such a slate means only, that after taking many such pictures and after superposing all of them to get ie picture, we see a perfectly sjfmmetric creature. [Pg.88]

Locate the rear transverse stabilizer rob in the corresponding position of carriage, symmetries the left and right during installation. [Pg.409]

FIGURE 4.28 The Icosahedron the symmetry axes (left) and the structure (right). [Pg.391]

FIGURE 4.42 The direct spinel structure (see the text for the details) left the view along the 4th order axes of symmetry right the view of packed structure after Heyes (1999). [Pg.413]

Figure 2. Structure of the Faujasite right part, a natural Faujasite with location of cations (l,r, II, ir and U) on symmetry axis. Left part, a protonated Faujasite with dots 1,2,3 and 4 showing the possible locations of -OH groups. Figure 2. Structure of the Faujasite right part, a natural Faujasite with location of cations (l,r, II, ir and U) on symmetry axis. Left part, a protonated Faujasite with dots 1,2,3 and 4 showing the possible locations of -OH groups.

See other pages where Symmetry right/left is mentioned: [Pg.467]    [Pg.23]    [Pg.650]    [Pg.705]    [Pg.92]    [Pg.101]    [Pg.13]    [Pg.23]    [Pg.243]    [Pg.48]    [Pg.229]    [Pg.588]    [Pg.105]    [Pg.55]    [Pg.48]    [Pg.71]    [Pg.47]    [Pg.53]    [Pg.264]    [Pg.391]   
See also in sourсe #XX -- [ Pg.48 ]




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LEFT

Left-and-right symmetry

Left/right

Right and Left-Handed Symmetry in Nature

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