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Rotating vector symbolism

The curl of a vector function (or rotation with symbol rot ) is a vector that is formally the cross product of the operator and the vector. For a vector V,... [Pg.810]

This presentation emphasizes the degeneracy that will exist physically. The symbol E is used for a 2-fold degenerate rep. The character tables contain an extra column labeled/ -, which indicates some functions that transform like the/th irreducible representation. The symbols/B c, , refer to rotations about the coordinate axes and may be regarded as rotational vectors. For example, is a clockwise rotational motion about 2 that is clearly invariant to rotations about the z axis. Thus z and R, transform in the same manner, and always in the manner of the totally symmetric. A, of the C groups. [Pg.72]

Screw rotation. The symmetry element is a screw axis. It can only occur if there is translational symmetry in the direction of the axis. The screw rotation results when a rotation of 360/1V degrees is coupled with a displacement parallel to the axis. The Hermann-Mauguin symbol is NM ( N sub M )-,N expresses the rotational component and the fraction M/N is the displacement component as a fraction of the translation vector. Some screw axes are right or left-handed. Screw axes that can occur in crystals are shown in Fig. 3.4. Single polymer molecules can also have non-crystallographic screw axes, e.g. 103 in polymeric sulfur. [Pg.15]

Fig. 9.8 The effect of reflection on (a) polar vectors representing translations (b) axial vectors representing rotations. In (b), the directions of the rotational-mode displacement vectors of the nuclei (symbolized by the curved lines) determine the directions of the axial vectors. Fig. 9.8 The effect of reflection on (a) polar vectors representing translations (b) axial vectors representing rotations. In (b), the directions of the rotational-mode displacement vectors of the nuclei (symbolized by the curved lines) determine the directions of the axial vectors.
Eq. (1.19) described the precession of M about the total magnetic field B using a coordinate system with fixed axes x, y, and z. Correspondingly, eq. (1.29) describes the magnetization vector M as it precesses about the effective field Beff [7] in a coordinate system rotating with frequency m = 2 7t v about the z axis and symbolized as the x , y, z frame of reference with the rotating unit vectors and k. [Pg.10]

Area III. In this part of the table, there will always be six symbols x, y, z, Rx, Ry,Rz, which may be taken as the three components of the translational vector (x, y, z) and the three rotations around the x, y, z axes (Rx, Ry, Rz). For the C2V character table, z appears in the row of A. This means that the z component of the translational vector has A symmetry. Similarly, the x and y components have B and B2 symmetry, respectively. The symmetries of rotations Rx, Ry, and Rz can be seen from this table accordingly. [Pg.181]

From the WET, Eq. [166], it is obvious that the reduced matrix element (RME) depends on the specific wave functions and the operator, whereas it is independent of magnetic quantum numbers m. The 3/ symbol depends only on rotational symmetry properties. It is related to the corresponding vector... [Pg.148]

Figure 2. Principal component biplot of rotated components 1 and 2 for mean descriptive analysis ratings (n=14 judges x 2 reps). Vectors for the aroma attributes, and the scores for the fifteen samples are shown. Open symbols indicate juice samples, while closed symbols indicate skin extracts. For sample codes, see Table II. Figure 2. Principal component biplot of rotated components 1 and 2 for mean descriptive analysis ratings (n=14 judges x 2 reps). Vectors for the aroma attributes, and the scores for the fifteen samples are shown. Open symbols indicate juice samples, while closed symbols indicate skin extracts. For sample codes, see Table II.
Rotations of 60°, 90°, 120°, or 180° are the only ones allowed,2 corresponding to six-, four-, three-, and twofold rotations. In addition, screw axes can occur, where the molecule is rotated by the same angles - 60°, 90°, 120°, 180° - and translated by a fraction of one of the lattice vectors a, b, or c. These have symbols like 21 (a 180° rotation followed by a translation of 1/2 of a lattice vector) or 43 (a 90° rotation followed by a translation of 3/4 of a lattice vector). These symmetry operators, lined up through the entire crystal, are the crystallographic symmetry operators. [Pg.53]

Subfamily B. These polytypes are described by orientational symbols with characters of alternating parity, i.e. by all-odd characters in the RTW symbol. Successive layers are related by (2 +l)x60° rotations. Only polytypes with an even number of layers appear in this subfamily. In addition, because layers with different orientational parity have an opposite x component of the stacking vector, Ev is ( ), (+) or -) and it is not possible to have a Class a polytype. [Pg.179]

Thethreeorthonormalbase vectors IEi, IE2, IE3 of type South , East", vertical" at the iniatial point Pa define the origin of the network (rotational degrees of freedom). The symbol has been used in order to refer the preferred directions to the North star a-ursae minoris. In emphasizing the reference of the orthonormal base vectors to the datum point Pa we make use of the notation... [Pg.441]


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See also in sourсe #XX -- [ Pg.150 ]




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