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Space groups of crystals

The English physicist William Barlow began as a London business man later he became interested in crystal structures and devoted his life to that study. In 1894, he published his findings of the 230 space groups. It is amazing that from consideration of symmetry three scientists in different countries arrived at the 230 space groups of crystals at about this time. Barlow then worked with ideas of close packing. He pictured the atoms in a crystal as spheres, which, under the influence... [Pg.2]

Table 11.20 Systematic Absences Used to Determine the Possible Space Groups of Crystal + X-Ray Beam ... Table 11.20 Systematic Absences Used to Determine the Possible Space Groups of Crystal + X-Ray Beam ...
Artur Moritz Sehoenflies (1853 1928), German mathematician and professor at the universities in Gottingen, Kdnigsherg, and Frankfurt am Main. Sehoenflies proved (independent of J.S. Fiodorow and W. Barlow) the existence of the complete set of 230 space groups of crystals. [Pg.1092]

In crystals, systems of equivalent points (orbits) are called Wyckoff positions. As we shall see, the total number of possible splittings of space of a crystal on systems of equivalent points is finite and for the three-dimensional periodicity case equals 230 (number of space groups of crystals).The various ways of filhng of equivalent points by atoms generate a huge (hundreds of thousands) number of real crystalline structures. [Pg.9]

Step 7. The computer determines the symmetry among the intensities of the reflections collected. The computer also looks for the absence or presence of intensity for certain classes of reflections. The computer determines which of 230 space groups the crystal belongs to from this information. [Pg.378]

Fig. 28 shows the crystal structure of Bi2Nb05F with a space group of I4/mmm - D. Bismuth ions, along with anions, form Bi202 type Bi2(0,F)2... [Pg.80]

According to investigations [215], the structure of Marignac s salt corresponds to the formula K2Ta203F6. The compound crystallizes in orthorhombic syngony, with a space group of Pnma - D, Z = 4. [Pg.89]

Depending on the size and packing (space group) of the asymmetric unit in the crystal and the resolution available, many tens of thousands of diffraction spots must be recorded to determine a structure. [Pg.282]

Analysis of the lanthanide-induced crystalline arrays by negative staining (Fig. 5) or freeze-fracture electron microscopy reveals obliquely oriented rows of particles, corresponding to individual Ca -ATPase molecules [119]. The unit cell dimensions for the gadolinium-induced Ca -ATPase crystals are a = 6. l A, b = 54.4 A and y = 111°. Similar cell constants were obtained for the crystals induced by lanthanum, praseodymium and calcium. The unit cell dimensions of the Ei crystals are consistent with a single Ca -ATPase monomer per unit cell. The space group of the Eptype crystals is PI [119], while that of the E2 crystals is P2 [88,90]. [Pg.73]

The traditional eharaeterisation of an electron density in a crystal amounts to a statement that the density is invariant under all operations of the space group of the crystal. The standard notation for sueh an operation is (Rim), where R stands for the point group part (rotations, reflections, inversion and combinations of these) and the direct lattice vector m denotes the translational part. When such an operation works on a vector r we get... [Pg.130]

The orbitals <]) j(k r) are Bloch functions labeled by a wave vector k in the first Brillouin zone (BZ), a band index p, and a subscript i indicating the spinor component. The combination of k and p. can be thought of as a label of an irreducible representation of the space group of the crystal. Thequantity n (k)is the occupation function which measures... [Pg.131]

The similarity of the structures of rutile, CaCl2 and marcasite also comes to light by comparison of their crystal structure data (Table 17.2). The space groups of CaCl2 and marcasite (both Pnnm) are subgroups of the space group of rutile. The tetragonal sym-... [Pg.199]

The occurrence of twinned crystals is a widespread phenomenon. They may consist of individuals that can be depicted macroscopically as in the case of the dovetail twins of gypsum, where the two components are mirror-inverted (Fig. 18.8). There may also be numerous alternating components which sometimes cause a streaky appearance of the crystals (polysynthetic twin). One of the twin components is converted to the other by some symmetry operation (twinning operation), for example by a reflection in the case of the dovetail twins. Another example is the Dauphine twins of quartz which are intercon-verted by a twofold rotation axis (Fig. 18.8). Threefold or fourfold axes can also occur as symmetry elements between the components the domains then have three or four orientations. The twinning operation is not a symmetry operation of the space group of the structure, but it must be compatible with the given structural facts. [Pg.223]

In this expression, G is the number of elements of the space group of the crystal, and / and n are the scattering power and number of the point random scatterers in... [Pg.17]

From the above properties it is evident that the set of operations t forms a group, J the space group of the crystal. If the translation operations are the primitive translations is r , ... [Pg.321]


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See also in sourсe #XX -- [ Pg.50 , Pg.51 , Pg.52 ]




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Crystal spacing

Crystals space groups

Group 230 space groups

Space group

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