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Rotation angles

The exact position of reflectors within the weld volume is calculated by means of the known probe position plus weld geometry and transferred to a true-to-scale representation of the weld (top view and side view). Repeated scanning of the same zone only overwrites the stored indications in cases where they reach a higher echo amplitude. The scanning movement of the probe is recorded in the sketch at the top, however, only if the coupling is adequate and the probe is situated within the permissible rotation angle. [Pg.777]

Figure 7 IN718 sample with segregation, SQUID-Signal versus rotation angle, scan radius is constant and equal to radial coordinate of segregation. Measurements are performed after demagnetization. Figure 7 IN718 sample with segregation, SQUID-Signal versus rotation angle, scan radius is constant and equal to radial coordinate of segregation. Measurements are performed after demagnetization.
T is a rotational angle, which determines the spatial orientation of the adiabatic electronic functions v / and )/ . In triatomic molecules, this orientation follows directly from symmetry considerations. So, for example, in a II state one of the elecbonic wave functions has its maximum in the molecular plane and the other one is perpendicular to it. If a treatment of the R-T effect is carried out employing the space-fixed coordinate system, the angle t appearing in Eqs. (53)... [Pg.520]

Fig. 1. The 2D graphene sheet is shown along with the vector which specifies the chiral nanotube. The chiral vector OA or Cf, = nOf + tnoi defined on the honeycomb lattice by unit vectors a, and 02 and the chiral angle 6 is defined with respect to the zigzag axis. Along the zigzag axis 6 = 0°. Also shown are the lattice vector OB = T of the ID tubule unit cell, and the rotation angle 4/ and the translation r which constitute the basic symmetry operation R = (i/ r). The diagram is constructed for n,m) = (4,2). Fig. 1. The 2D graphene sheet is shown along with the vector which specifies the chiral nanotube. The chiral vector OA or Cf, = nOf + tnoi defined on the honeycomb lattice by unit vectors a, and 02 and the chiral angle 6 is defined with respect to the zigzag axis. Along the zigzag axis 6 = 0°. Also shown are the lattice vector OB = T of the ID tubule unit cell, and the rotation angle 4/ and the translation r which constitute the basic symmetry operation R = (i/ r). The diagram is constructed for n,m) = (4,2).
Figure 12.16), can insert between the stacked base pairs of DNA. The bases are forced apart to accommodate these so-called intercalating agents, causing an unwinding of the helix to a more ladderlike structure. The deoxyribose-phosphate backbone is almost fully extended as successive base pairs are displaced 0.7 nm from one another, and the rotational angle about the helix axis between adjacent base pairs is reduced from 36° to 10°. [Pg.370]

Normally the orbitals are real, and the unitary transformation becomes an orthogonal transformation. In the case of only two orbitals, the X matrix contains the rotation angle a, and the U matrix describes a 2 by 2 rotation. The connection between X and U is illustrated in Chapter 13 (Figure 13.2) and involves diagonalization of X (to give eigenvalues of ia), exponentiation (to give complex exponentials which may be witten as cos a i sin a), follow by backtransformation. [Pg.69]

In the general case the X matrix contains rotational angles for rotating all pairs of orbitals. [Pg.69]

These elements can be reduced to zero by choosing a proper rotational angle. [Pg.311]

As the most notable contribution of ab initio studies, it was revealed that the different modes of molecular deformation (i.e. bond stretching, valence angle bending and internal rotation) are excited simultaneously and not sequentially at different levels of stress. Intuitive arguments, implied by molecular mechanics and other semi-empirical procedures, lead to the erroneous assumption that the relative extent of deformation under stress of covalent bonds, valence angles and internal rotation angles (Ar A0 AO) should be inversely proportional to the relative stiffness of the deformation modes which, for a typical polyolefin, are 100 10 1 [15]. A completly different picture emerged from the Hartree-Fock calculations where the determined values of Ar A0 AO actually vary in the ratio of 1 2.4 9 [91]. [Pg.108]

Fig. 7. Molecular model of cyclododecane in the (gag)4 conformation of the crystalline state according to Dunitz and Shearer (Ref. 12>). The numbers at the bonds indicate the rotational angles... Fig. 7. Molecular model of cyclododecane in the (gag)4 conformation of the crystalline state according to Dunitz and Shearer (Ref. 12>). The numbers at the bonds indicate the rotational angles...
Fig. 9. Molecular model of the crystal conformation of cyclotetraeicosane at —160 °C according to P. Groth, ref. 19. The numbers at the bonds give the rotational angles. The assignment of the CP-MAS 13C-NMR shifts to conformational four bond sequences is given at the carbon atoms of the upper left corner... Fig. 9. Molecular model of the crystal conformation of cyclotetraeicosane at —160 °C according to P. Groth, ref. 19. The numbers at the bonds give the rotational angles. The assignment of the CP-MAS 13C-NMR shifts to conformational four bond sequences is given at the carbon atoms of the upper left corner...
Figure 2. Radical cations (polarons) and dications (bipolarons) obtained by oxidation of the neutral chain. The rotated angles and counter-ions needed to retain electroneutrality are not shown. Figure 2. Radical cations (polarons) and dications (bipolarons) obtained by oxidation of the neutral chain. The rotated angles and counter-ions needed to retain electroneutrality are not shown.
Fig. 5 —The relation between the rotated angle of reflection beam (a) and the torsional angle of cantilever ( /), (1-rotated angle of the reflection beam, a 2-incident angle, y 3-torsional angle of the cantilever, / 4-reflection surface before torsion of the cantilever 5-reflection surface after torsion of the cantilever). Fig. 5 —The relation between the rotated angle of reflection beam (a) and the torsional angle of cantilever ( /), (1-rotated angle of the reflection beam, a 2-incident angle, y 3-torsional angle of the cantilever, / 4-reflection surface before torsion of the cantilever 5-reflection surface after torsion of the cantilever).
The incident angle is a constant for this equipment, y = 15°. The torsional angle i, and the rotated angle a of the reflection ray are both infinitesimals. The formula can be simpli-... [Pg.190]

Transverse moving head of four-quadrant position detectors (Fig. 2), precise measuring lateral displacement which corresponds to lateral voltage F/ when it varies at the linear range of 10 V, thus we can compute the rotated angle a of the reflection ray ... [Pg.190]


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Rotational angle

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