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Polar angle

Consider the case of two neutral, linear, dipolar molecules, such as HCN and KCl, in a coordinate system with its origin at the CM of molecule A and the z-axis aligned with the intemiolecular vector r pointing from the CM of A to the CM of B. The relative orientation of the two molecules is uniquely specified by their spherical polar angles 0, 03 and the difierence <]) = - <])3 between their azimuthal angles. The leading temi in the... [Pg.189]

The magnitudes of e i =1, )contam the Fresnel factors from equation Bl.5,34. equation B1,5,35 and equation B 1,5.36. which depend on the incident, reflected and polarization angles. Experimentally, one approach is to fix the input polarization and adjust the analyser to obtain a null in the SFl signal [ ]. By choosing distinct configurations such that the corresponding tliree equations from equation B 1.5.40 are linearly independent, the relative values of Xs lim = inferred. This method has... [Pg.1283]

Figure Bl.5.8 Random distribution of (a) non-chiral adsorbates that gives rise to a surfaee having effeetive oo m-synnnetry (b) ehiral moleeules that gives rise to effeetive oo-synnnetry. (e) SH intensity versus the angle of an analyser for a raeemie (squares) and a non-raeemie (open eireles) monolayer of ehiral moleeules. The pump beam was p-polarized the SH polarization angles of 0° and 90° eorrespond to s- and p-polarization, respeetively. (From [70].)... Figure Bl.5.8 Random distribution of (a) non-chiral adsorbates that gives rise to a surfaee having effeetive oo m-synnnetry (b) ehiral moleeules that gives rise to effeetive oo-synnnetry. (e) SH intensity versus the angle of an analyser for a raeemie (squares) and a non-raeemie (open eireles) monolayer of ehiral moleeules. The pump beam was p-polarized the SH polarization angles of 0° and 90° eorrespond to s- and p-polarization, respeetively. (From [70].)...
Three rotational diffusion coefficients, two polar angles 0 and T... [Pg.1505]

Figure Cl.5.14. Fluorescence images of tliree different single molecules observed under the imaging conditions of figure Cl.5.13. The observed dipole emission patterns (left column) are indicative of the 3D orientation of each molecule. The right-hand column shows the calculated fit to each observed intensity pattern. Molecules 1, 2 and 3 are found to have polar angles of (0,( ))=(4.5°,-24.6°), (-5.3°,51.6°) and (85.4°,-3.9°), respectively. Reprinted with pennission from Bartko and Dickson [148]. Copyright 1999 American Chemical Society. Figure Cl.5.14. Fluorescence images of tliree different single molecules observed under the imaging conditions of figure Cl.5.13. The observed dipole emission patterns (left column) are indicative of the 3D orientation of each molecule. The right-hand column shows the calculated fit to each observed intensity pattern. Molecules 1, 2 and 3 are found to have polar angles of (0,( ))=(4.5°,-24.6°), (-5.3°,51.6°) and (85.4°,-3.9°), respectively. Reprinted with pennission from Bartko and Dickson [148]. Copyright 1999 American Chemical Society.
From these relations it follows that is related to the angular momentum modulus, and that the pairs of angle a, P and y, 8 are the azimuthal, and the polar angle of the (J ) and the (L ) vector, respectively. The angle is associated with the relative orientation of the body-fixed and space-fixed coordinate frames. The probability to find the particular rotational state IMK) in the coherent state is... [Pg.244]

Fig. 11.22 Small surface elements can be created on the van der Waals surface of an atom using constant increments of the polar angles, 6 and 0. Fig. 11.22 Small surface elements can be created on the van der Waals surface of an atom using constant increments of the polar angles, 6 and 0.
Figure 2 Experimental data from an early stage of CO adsorbed on Fe (001) known as the GC3 state polar scans (a) of the C 1s-0 Is Intansity ratio taken in two Fe (001) azimuthal planes, the (100) and the (ITO) (the C Is and O Is electron kinetic energies are 1202 aV and 955 aV, respectively) C Is azimuthal scan (b) taken at the polar angle of maximum intensity in (a) and geometry (c) deduced from the data. Figure 2 Experimental data from an early stage of CO adsorbed on Fe (001) known as the GC3 state polar scans (a) of the C 1s-0 Is Intansity ratio taken in two Fe (001) azimuthal planes, the (100) and the (ITO) (the C Is and O Is electron kinetic energies are 1202 aV and 955 aV, respectively) C Is azimuthal scan (b) taken at the polar angle of maximum intensity in (a) and geometry (c) deduced from the data.
We now discuss the annular tautomerism of azoles. For 5-phenyltetra-zole, the 2//-tautomer was found predominant in polyvinyl alcohol film (based on the determination of polarization angles of electronic transition... [Pg.49]

PoLar-licht, n. aurora polaris. -rohre, /. electrode tube, -stem, m. poleatar, -winkel, m. polar angle. [Pg.344]

In polar coordinates (Figure 1-34), r f(0), where r is the radius vector and 0 is the polar angle, and... [Pg.40]

Polar angle defined with respect to a structural unit... [Pg.82]

Here, Yx m( j) denotes a spherical harmonic, coj represents the spherical polar angles made by the symmetry axis of molecule i in a frame containing the intermolecular vector as the z axis. The choice of the x and y axes is arbitrary because the product of the functions being averaged depends on the difference of the azimuthal angles for the two molecules which are separated by distance r. At the second rank level the independent correlation coefficients are... [Pg.78]

C, 0.25 nm molecule in the coexistence region between the liquid-expanded and the liquid-condensed (L2) phases (b) BAM image of stearic acid at 22°C, 0.60 nm molecule in the coexistence region between the gas (G) and the hquid-condensed (L2) phases. In each of these images, the polarizer angle has been set to 60°. The subphase is milh-Q water acidified to pH 1.8 with HCl. The scale bar in the lower left of each image is 450 p,m. [Pg.66]

In humid environments, the ellipsometry results of Beaglehole and Christenson [71] indicate that a film is formed with an average thickness of 2 A when the relative humidity (RH) is 50%. As discussed earlier, however, the lateral resolution of ellipsometry is limited by the size of the light spot on the sample, typically several tens of micrometers. In addition, thickness values are obtained from the measured changes in polarization angle by... [Pg.269]

We represent the four-atom problem in terms of diatom-diatom Jacobi coordinates R, the vector between the AB and CD centers of mass, and rj and r2, the AB and CD bond vectors. In a body-fixed coordinate system [19,20] with the z-axis chosen to R, only six coordinate variables need be considered, which we choose to be / , ri, and ra, the magnitudes of the Jacobi vectors, and the angles 01, 02, and (j). Here 0, denotes the usual polar angle of r, relative to the z-axis, and 4> is the difference between the azimuthal angles for ri and r2 (i.e., a torsion angle). [Pg.11]

Fig. 4.16 Definition of the polar angles 9, c(). k is the wave vector of the emitted y-ray. The z-axis may be defined by the direction of a magnetic field... Fig. 4.16 Definition of the polar angles 9, c(). k is the wave vector of the emitted y-ray. The z-axis may be defined by the direction of a magnetic field...
From (4.56) and Table 4.3, we derive the relative intensity ratios 3 2 1 1 2 3 for the hyperfine components of a Zeeman pattern of a powder sample. The transition probability for the case of the polar angle 6 = Oq can readly be calculated by integrating (4.56) only over the azimuthal angle (j). One obtains a factor (1 + cos 0o)/2 and sin 0o for m = 1 and m = 0, respectively, which are multiplied by the square of the Clebsch-Gordan coefficients. As a consequence of the angular correlation of the transition probabilities the second and fifth hyperfine components (Fig. 4.17) disappear if the direction k of the y-rays and the magnetic field H are parallel (0q = 0). [Pg.116]

Figure 4. Kinematics of the solid-state EMS spectrometer [11]. (a) The polar angles made by kf and k, with respect to the incident (z) direction are Of = 14° and 6% = 76°. In (b) is shown a typical sample membrane relative to the electron trajectories. The surface sensitivity is largely determined by the escape depth of the 1.2 keV electrons ( 2 nm) and is indicated by the shaded area. [Pg.211]

Overall mass-transfer rates at a sphere in forced flow, and mass-transfer rate distribution over a sphere as a function of the polar angle have been measured by Gibert, Angelino, and co-workers (G2, G4a) for a wide range of Reynolds numbers. The overall rate dependence on Re exhibited two distinct regimes with a sharp transition at Re = 1250. Local mass-transfer rates were deduced from measurements in which the sphere was progressively coated by an insulator, starting from the rear. [Pg.263]


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See also in sourсe #XX -- [ Pg.114 ]

See also in sourсe #XX -- [ Pg.52 ]




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