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Electric polarization vector

Figure 44. Absolute atomic arrangement of glycine I in TGS (see Figure 43) and the direction of the electric polarization vector p for the two enantiomorphous states (a) and (b) (ref. 110). Figure 44. Absolute atomic arrangement of glycine I in TGS (see Figure 43) and the direction of the electric polarization vector p for the two enantiomorphous states (a) and (b) (ref. 110).
Here E, D, and P represent, respectively, the electric field, electric induction (or displacement), and electric polarization vectors P (D - )/4x. The integration must be carried out over all space penetrated by the electrostatic field. Equation (5.6.1), while correct, is awkward in several respects. First, there is the need to integrate over all space, including the region outside the system of interest. In the presence of a medium, the electric lines of force not only are present within the specimen, but also bulge out in all directions away from the system these effects must be included in (5.6.1). Second, there is a tendency in the literature to associate the first term in (5.6.1b) with the establishment of the electric field in free space, and the second term with the reaction of the medium to the electric field. This is wrong The quantity D is subject to direct experimental control because it is linked by Maxwell s equation to the presence of free charges by contrast, E is in part a reaction field that also includes the... [Pg.493]

In Eq. 2, D is the electric displacement or electric flux density vector, E is the electric field vector, P is the electric polarization vector, and is the permittivity of vacuum. In many isotropic materials the induced polarization is directly proportional to the applied field strength, except for the case of very high fields. We can write [71]... [Pg.545]

Fig. 19. NEXAFS images acquired at 286.7 eV of a 99/1 (w/w) PET/Vectra blend subjected to post-milling melt pressing. Images (A) and (B) have been converted to optical density. In images (A) and (B), the electric polarization vector E is rotated by 90° with respect to each other, as indicated. Changes in the relative intensity in these images are primarily due to anisotropic molecular orientation. The ratio of these images (C) reveals the linear dichroism of the specimen. Small Vectra domains appear gray and possess no discernible orientation, whereas the large dispersion exhibits a measurable degree of molecular orientation (black and white areas) because of the nematic nature of this liquid crystalline poljrmer. (Data acquired with the Stony Brook STXM.) Reproduced from Ref 144. Fig. 19. NEXAFS images acquired at 286.7 eV of a 99/1 (w/w) PET/Vectra blend subjected to post-milling melt pressing. Images (A) and (B) have been converted to optical density. In images (A) and (B), the electric polarization vector E is rotated by 90° with respect to each other, as indicated. Changes in the relative intensity in these images are primarily due to anisotropic molecular orientation. The ratio of these images (C) reveals the linear dichroism of the specimen. Small Vectra domains appear gray and possess no discernible orientation, whereas the large dispersion exhibits a measurable degree of molecular orientation (black and white areas) because of the nematic nature of this liquid crystalline poljrmer. (Data acquired with the Stony Brook STXM.) Reproduced from Ref 144.
As in previous chapters we work in the continuum limit employing quantities averaged over macroscopically infinitesimal volume elements and disregarding microscopic local variations associated with the molecular structure (see Brown 1956). These considerations will be limited to processes sufficiently slow to restrict the treatment to time independent or quasistatic fields. The validity of Maxwell s equations of electrostatics is presupposed. The basic electric state variables are the electric field strength vector E, the electric flux density (or electric displacement) vector D, and the electric polarization vector P, related by... [Pg.55]

The electrical induction D corresponds, in fact, to a very particiilar measurement of the electrical field D is actually the electrical field measured in a flattened cylindrical cavity, whose axis runs in the same direction as the electrical polarization vector P. ... [Pg.50]

State I ) m the electronic ground state. In principle, other possibilities may also be conceived for the preparation step, as discussed in section A3.13.1, section A3.13.2 and section A3.13.3. In order to detemiine superposition coefficients within a realistic experimental set-up using irradiation, the following questions need to be answered (1) Wliat are the eigenstates (2) What are the electric dipole transition matrix elements (3) What is the orientation of the molecule with respect to the laboratory fixed (Imearly or circularly) polarized electric field vector of the radiation The first question requires knowledge of the potential energy surface, or... [Pg.1059]

Since the electric field is a polar vector, it acts to break the inversion synnnetry and gives rise to dipole-allowed sources of nonlinear polarization in the bulk of a centrosymmetric medium. Assuming that tire DC field, is sufficiently weak to be treated in a leading-order perturbation expansion, the response may be written as... [Pg.1280]

Information about the properties of the sample are contained in the complex ratio, p, of the Fresnel coefficients of reflection of the parallel (rp) and perpendicular (rg) incident plane polarized electrical field vectors. [Pg.266]

A powerful characteristic of RAIR spectroscopy is that the technique can be used to determine the orientation of surface species. The reason for this is as follows. When parallel polarized infrared radiation is specularly reflected off of a substrate at a large angle of incidence, the incident and reflected waves combine to form a standing wave that has its electric field vector (E) perpendicular to the substrate surface. Since the intensity of an infrared absorption band is proportional to / ( M), where M is the transition moment , it can be seen that the intensity of a band is maximum when E and M are parallel (i.e., both perpendicular to the surface). / is a minimum when M is parallel to the surface (as stated above, E is always perpendicular to the surface in RAIR spectroscopy). [Pg.251]

Polarized light (Section 7.4) Light in which the electric held vectors vibrate in a single plane. Polarized light is used in measuring optical activity. [Pg.1291]

Polarized light is light that has the electric field vector of all of the energy vibrating in the same plane. Looking into the end of a beam of polarized light one would see the electric field vectors as parallel or coincident lines. [Pg.231]

Fig. 3—Measurement of surface by HDI surface reflectance analyzer. In electromagnetic radiation (light), the polarization direction is defined as the direction of the electric field vector. The incident polarization of the light can be controlled. The instrument uses a variety of detectors to analyze the reflected polarization state of the light. (U.S. Patent 6,134,011). (a) Plane of the disk The SRA uses a fixed 60 degree (from the surface normal) angle of incidence. The plane of incidence is the same as the paper plane (b) Pit on a surface detected by reflected light channels of HDI instrument (c) Scratches on disk surface measured by HDI surface reflectance analyzer (d) Particles on the surface of disk detected by reflected light (black spot) and by scattered light (white spot) [8]. Fig. 3—Measurement of surface by HDI surface reflectance analyzer. In electromagnetic radiation (light), the polarization direction is defined as the direction of the electric field vector. The incident polarization of the light can be controlled. The instrument uses a variety of detectors to analyze the reflected polarization state of the light. (U.S. Patent 6,134,011). (a) Plane of the disk The SRA uses a fixed 60 degree (from the surface normal) angle of incidence. The plane of incidence is the same as the paper plane (b) Pit on a surface detected by reflected light channels of HDI instrument (c) Scratches on disk surface measured by HDI surface reflectance analyzer (d) Particles on the surface of disk detected by reflected light (black spot) and by scattered light (white spot) [8].
FIGURE 27.23 Electric (E) and magnetic (H) vectors in a linearly polarized light wave. The plane of polarization contains the electric field vectors in space. At a fixed focation, the tip of the electric vector traces a straight line as a function of time. (From Muller, 1973, with permission from Wiley-VCH.)... [Pg.491]

Another very important property of synchrotron radiation is its very high degree of polarization. The radiation is predominantly polarized with the electric field vector parallel to the acceleration... [Pg.271]


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