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Fourfold symmetry

Like the photosynthetic reaction center and bacteriorhodopsin, the bacterial ion channel also has tilted transmembrane helices, two in each of the subunits of the homotetrameric molecule that has fourfold symmetry. These transmembrane helices line the central and inner parts of the channel but do not contribute to the remarkable 10,000-fold selectivity for K+ ions over Na+ ions. This crucial property of the channel is achieved through the narrow selectivity filter that is formed by loop regions from thefour subunits and lined by main-chain carbonyl oxygen atoms, to which dehydrated K ions bind. [Pg.248]

The physics underlying Eqs. (74-76) is quite simple. A solidifying front releases latent heat which diffuses away as expressed by Eq. (74) the need for heat conservation at the interface gives Eq. (75) Eq. (76) is the local equilibrium condition at the interface which takes into account the Gibbs-Thomson correction (see Eq. (54)) K is the two-dimensional curvature and d Q) is the so-called anisotropic capillary length with an assumed fourfold symmetry. [Pg.889]

At present only low resolution (>30A) structures, all derived from single particle analysis of images from electron microscopy, are available for the entire DP3R. These structures differ in their details, but all show a roughly square structure with fourfold symmetry and lateral dimensions of about 20 nm (Fig. 2). [Pg.664]

Figure 7.11 Field ion microscopy image of a platinum tip. As Pt has the fee structure, the fourfold symmetry of the picture implies that the center corresponds to a (100) facet. Dark areas near the four comers are (111) facets (from Muller [26]). [Pg.194]

The values for the dipoles, polarizabilities, and hyperpolarizabilities of the H2 series were obtained using (a) a 16-term basis with a fourfold symmetry projection for the homonuclear species and (b) a 32-term basis with a twofold symmetry projection for the heteronuclear species. These different expansion lengths were used so that when combined with the symmetry projections the resulting wave functions were of about the same quality, and the properties calculated would be comparable. A crude analysis shows that basis set size for an n particle system must scale as k", where k is a constant. In our previous work [64, 65] we used a 244-term wave function for the five-internal-particle system LiH to obtain experimental quality results. This gives a value of... [Pg.457]

Figure 4.7 shows top-down views of the fee (001), (111), and (110) surfaces. These views highlight the different symmetry of each surface. The (001) surface has fourfold symmetry, the (111) surface has threefold symmetry, and the (110) has twofold symmetry. These three fee surfaces are all atomically flat in the sense that on each surface every atom on the surface has the same coordination and the same coordinate relative to the surface normal. Collectively, they are referred to as the low-index surfaces of fee materials. Other crystal structures also have low-index surfaces, but they can have different Miller indices than for the fee structure. For bcc materials, for example, the surface with the highest density of surface atoms is the (110) surface. [Pg.90]

The two wavefunctions, P l and F2, should have the same amplitude because of the fourfold symmetry. A direct calculation gives the charge density ... [Pg.130]

The symbols for plane groups, the Hermann-Mauguin symbol, have been the standard in crystallography. The first place indicates the type of lattice, p indicates primitive, and c indicates centered. The second place indicates the axial symmetry, which has only 5 possible vales, 1-, 2-, 3-, 4-, and 6-fold. For the rest, the letter m indicates a symmetry under a mirror reflection, and the letter g indicates a symmetry with respect to a glide line, that is, one-half of the unit vector translation followed by a mirror reflection. For example, the plane group pAmm means that the surface has fourfold symmetry as well as mirror reflection symmetries through both x and y axes. [Pg.358]

Vc must be unchanged by any symmetry operation of this octahedral group. First, we note that there is a center of symmetry, and therefore Vc must remain unchanged when 6 and 0 are replaced by 7t — 0 and 0 + 7r. This is true only of spherical harmonics with even values of /, and therefore we only need terms with /= 0, 2, and 4 in our expansions. Second, we note that there is a fourfold symmetry axis along the z axis therefore, Vc must remain unchanged when is replaced by 0 + 77. Since T/m(0,0) is of the form... [Pg.102]

Note that, for a crystal field with no three- or fourfold symmetry axes (D and 0), the spin degeneracy is completely removed by the spin-spin interaction even in the absence of a magnetic field. This is a characteristic... [Pg.126]

Figure 10. Projection of entire unit cell on the xy plane. Filled squares indicate centers of fourfold symmetry, while the small, dark, unfilled circles are inversion points. Small hexagons are H20 positions dotted lines are possible hydrogen bonds. Three-dimensional distances are indicated in... Figure 10. Projection of entire unit cell on the xy plane. Filled squares indicate centers of fourfold symmetry, while the small, dark, unfilled circles are inversion points. Small hexagons are H20 positions dotted lines are possible hydrogen bonds. Three-dimensional distances are indicated in...
Example 2. This example shows that the symmetry of the pattern can be less than that of the object used to create it. The blocks may be perfectly square, but the pattern does not have fourfold symmetry. Again, a net of reflection lines is perhaps most obvious and, of course, there are twofold axes at their intersections. If this were all, we would have pmm symmetry. However, it can be seen that the array is centered, and closer inspection will show that there are horizontal and vertical glide lines and an additional set of twofold axes, making this an example of cmm symmetry. [Pg.368]

Worked Example Why is an A-centered tetragonal lattice not possible Because centering only on the A faces (or only on the B faces) would destroy the fourfold symmetry and hence the lattice would not be tetragonal. The question of why centering on both the A and B faces is also disallowed is left as an exercise for the reader. [Pg.372]

Tetragonal. The essential requirement here is fourfold symmetry, either 4 or 4. The only symmetry elements that can be added are those perpendicular or parallel to 4 or 4, so as not to generate additional 4 or 4 axes otherwise, the symmetry would increase to some type of cubic symmetry. [Pg.381]

Preservation of fourfold symmetry along the 27, X2, and xs axes requires that any flux components in directions perpendicular to the gradients be zero. Therefore,... [Pg.95]


See other pages where Fourfold symmetry is mentioned: [Pg.924]    [Pg.2617]    [Pg.46]    [Pg.233]    [Pg.245]    [Pg.663]    [Pg.555]    [Pg.319]    [Pg.320]    [Pg.320]    [Pg.321]    [Pg.186]    [Pg.164]    [Pg.165]    [Pg.38]    [Pg.20]    [Pg.137]    [Pg.266]    [Pg.110]    [Pg.194]    [Pg.75]    [Pg.153]    [Pg.15]    [Pg.75]    [Pg.508]    [Pg.250]    [Pg.13]    [Pg.113]    [Pg.142]    [Pg.35]    [Pg.1114]    [Pg.74]    [Pg.75]   
See also in sourсe #XX -- [ Pg.415 , Pg.448 ]

See also in sourсe #XX -- [ Pg.415 , Pg.448 ]




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