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Liquid crystal and polymer

Simoni F 1997 Nonlinear Optical Properties of Liquid Crystals and Polymer-Dispersed Liquid Crystals (Singapore World Scientific)... [Pg.2571]

P.-G. de Gennes (College de France, Paris) discovery that methods developed for studying order phenomena in simple systems can be generalized to more complex forms of matter, in particular to liquid crystals and polymers. [Pg.1304]

Confocal fluorescence microscopy has been extensively used in cell biology. Single living cells can indeed be studied by this technique visualization of organelles, distribution of electrical potential, pH imaging, Ca2+ imaging, etc. (Lemasters, 1996). Interesting applications in chemistry have also been reported in the fields of colloids, liquid crystals and polymer blends. [Pg.355]

Scharf, T. 2007. Polarized Light in Liquid Crystals and Polymers. Wiley, Hoboken, NJ. [Pg.623]

One of the points made in Schwenz and Moore was that the physical chemistry laboratory should better reflect the range of activities found in current physical chemistry research. This is reflected in part by the inclusion of modem instrumentation and computational methods, as noted extensively above, but also by the choice of topics. A number of experiments developed since Schwenz and Moore reflect these current topics. Some are devoted to modem materials, an extremely active research area, that I have broadly construed to include semiconductors, nanoparticles, self-assembled monolayers and other supramolecular systems, liquid crystals, and polymers. Others are devoted to physical chemistry of biological systems. I should point out here, that with rare exceptions, I have not included experiments for the biophysical chemistry laboratory in this latter category, primarily because the topics of many of these experiments fall out of the range of a typical physical chemistry laboratory or lecture syllabus. Systems of environmental interest were well represented as well. [Pg.128]

Materials Nanoparticles, Self-Assembled Monolayers Supramolecular Systems, Liquid Crystals and Polymers... [Pg.128]

Statistical mechanics was originally formulated to describe the properties of systems of identical particles such as atoms or small molecules. However, many materials of industrial and commercial importance do not fit neatly into this framework. For example, the particles in a colloidal suspension are never strictly identical to one another, but have a range of radii (and possibly surface charges, shapes, etc.). This dependence of the particle properties on one or more continuous parameters is known as polydispersity. One can regard a polydisperse fluid as a mixture of an infinite number of distinct particle species. If we label each species according to the value of its polydisperse attribute, a, the state of a polydisperse system entails specification of a density distribution p(a), rather than a finite number of density variables. It is usual to identify two distinct types of polydispersity variable and fixed. Variable polydispersity pertains to systems such as ionic micelles or oil-water emulsions, where the degree of polydispersity (as measured by the form of p(a)) can change under the influence of external factors. A more common situation is fixed polydispersity, appropriate for the description of systems such as colloidal dispersions, liquid crystals, and polymers. Here the form of p(cr) is determined by the synthesis of the fluid. [Pg.49]

J. M. Garcia Fernandez, A. Gadelle, and J. Defaye, Difructose dianhydrides from sucrose and fructooligosaccharides and their use as building blocks for the preparation of amphiphiles, liquid crystals and polymers, Carbohydr. Res., 265 (1994) 249-269. [Pg.285]

Polymer-based photochromic systems have been studied extensively and are attractive in terms of practical applications because of their advantages of stability and processability. A number of reviews and articles dealing with various aspects of photochromic polymers and photoactive biomaterials have been published. 68 Chiral photochromic peptides are discussed in Chapter 13, and photochromic liquid crystals and polymers for holographic data storage and nonlinear optics have been reviewed. 69 Specific stereochemical effects in chiral photoresponsive polymers include ... [Pg.152]

Paricaud, P., Galindo, A., and Jackson, G., Recent advances in the nse of the SAFT approach in describing electrolytes, interfaces, liquid crystals and polymers. Fluid Phase Equilibria, 87, 194—197, 2002. [Pg.743]

It should be noted that any defects and imperfection in structure and orientation would give rise to rather coarse points and doughnut-shaped zones in the reciprocal lattice rather than clearly defined points and circles. This is the case for oriented liquid crystals and polymer fibers. Diffused diffraction patterns are therefore obtained for these specimens. [Pg.232]

Since the liquid crystal forms the continuous phase of the binary mixture, we are only interested in a small part of the total phase diagram. Weight fractions of the liquid crystal in the range 0.9 to 1 were used to determine the partial phase diagram of the mixture which is shown in Fig. 2. The system forms an isotropic (I) phase at high temperature, and a diphasic equilibrium between an isotropic and a nematic phase (N-i-I) at low temperature. A nematic domain (N) is found at intermediate temperatures and low silicone oil concentrations. As pointed out in the experimental section, the existence of this nematic domain has some importance prior to quenching the system to the diphasic region. The present mixture exhibits classical features usually observed in other mixtures of nematic liquid crystals and polymers or isotropic fluids [29,30]. [Pg.180]

F. Simoni, Nonlinear optical properties of liquid crystals and polymer dispersed liquid crystals World Scientific, Singapore 1997. [Pg.120]

The liquid crystalline material in the LCD is not necessarily a LCP. However, in order to fix the liquid crystalline material conventional polymers are used for embedding and LCP are also used. Side chain LCPs combine the properties of liquid crystals and polymers with flexible main chains. Since the liquid crystal moieties are fixed on the backbone of the main chains of the polymer, this type of liquid crystals may not flow away, as it may be the case in monomeric liquid crystals. [Pg.540]

Link 4. Comparison to Experiment for Liquid Crystals Liquid crystals and polymer glasses are really two faces of the same coin. In both cases e transition occurs because of a geometrical frustration arising from the stiffness of the chain. [Pg.26]

Morphology of Composites of Low-Molar-Mass Liquid Crystals and Polymer Networks... [Pg.507]

Hess, M. and Lopez, B. (1997) Phase diagrams of polymer liquid crystals and polymer liquid crystal blends relation to mechanical properties, in this volume. [Pg.209]

Chilaya, G., Hank, G., Koswig, H.D., Sikhamlidze, D. Electric-field controlled color effect in cholesteric liquid crystals and polymer-dispersed cholesteric liquid crystals. J. Appl. Phys. 80, 1907-1909 (1996)... [Pg.378]

Scharf, T. (2007). Polarized light in liquid crystals and polymers. Wiley, ISBN 978-0-471-740643, New Jersey... [Pg.196]

Ferroelectric crystals (especially oxides in the form of ceramics) are important basic materials for technological applications in capacitors and in piezoelectric, pyroelectric, and optical devices. In many cases their nonlinear characteristics turn out to be very useful, for example in optical second-harmonic generators and other nonlinear optical devices. In recent decades, ceramic thin-film ferroelectrics have been utilized intensively as parts of memory devices. Liquid crystal and polymer ferroelectrics are utilized in the broad field of fast displays in electronic equipment. [Pg.903]

Rg. r.5 -If Number of ferroelectric substances known at the end of each year. The solid line represents aU ferro-electrics, including hqnid crystals and polymers. For liquid crystals and polymers, each gronp of homolognes is connted as one substance. The dashed line represents ferroelectric hquid crystals and polymers alone. Figure prepared by Prof. K. Deguchi... [Pg.906]

In the Landolt-Bdmstein data collection, ferroelectric and antiferroelectric substances are classified into 72 families according to their chemical composition and their crystallographic structure. Some substances which are in fact neither ferroelectric nor antiferroelectric but which are important in relation to ferroelectricity or anti-ferroelectricity, for instance as an end material of a solid solution, are also included in these families as related substances. This subsection surveys these 72 families of ferroelectrics presented in Landolt-Bornstein Vol. III/36 (LB III/36). Nineteen of these families concern oxides [5.1,2], 30 of them concern inorganic crystals other than oxides [5.3], and 23 of them concern organic crystals, liquid crystals, and polymers [5.4]. Table 4.5-1 lists these families and gives some information about each family. Substances classified in LB 111/36 as miscellaneous crystals (outside the families) are not included. [Pg.909]

Family Nr. Inorganic Crystals Oxides [5.1,2] Name Family Nr. Inoi anic Crystals other than Oxides [5.3] Name Orgi Family Nr. uiic Crystals, Liquid Crystals, and Polymers [5.4] Name... [Pg.910]

Table A..5-1 The 72 families of ferroelectric materials. The number assigned to each family corresponds to the number used in LB III/36. The numbers in parentheses (A sub>. f+a ) after the family name serve the purpose of conveying some information about the size and importance of the family. The numbers indicate the following A sub the number of pure substances (ferroelectric, antiferroelectric, and related substances) which are treated as members of this family in LB III/36 A f+A the number of ferroelectric and antiferroelectric substances which are treated as members of this family in LB III/36 n, the number of representative substances from this family whose properties are surveyed in Sect. 4.5.4. For some of these families, additional remarks are needed for instance, because the perovskite-type oxide family has many members and consists of several subfamilies because the liquid crystal and polymer families have very specific properties compared with crystalline ferroelectrics and because the traditional names of some families are apt to lead to misconceptions about their members. Such families are marked by letters a-m following the parentheses, and remarks on these families are given under the corresponding letter in the text in Sect. 4.5.3.1... Table A..5-1 The 72 families of ferroelectric materials. The number assigned to each family corresponds to the number used in LB III/36. The numbers in parentheses (A sub>. f+a ) after the family name serve the purpose of conveying some information about the size and importance of the family. The numbers indicate the following A sub the number of pure substances (ferroelectric, antiferroelectric, and related substances) which are treated as members of this family in LB III/36 A f+A the number of ferroelectric and antiferroelectric substances which are treated as members of this family in LB III/36 n, the number of representative substances from this family whose properties are surveyed in Sect. 4.5.4. For some of these families, additional remarks are needed for instance, because the perovskite-type oxide family has many members and consists of several subfamilies because the liquid crystal and polymer families have very specific properties compared with crystalline ferroelectrics and because the traditional names of some families are apt to lead to misconceptions about their members. Such families are marked by letters a-m following the parentheses, and remarks on these families are given under the corresponding letter in the text in Sect. 4.5.3.1...

See other pages where Liquid crystal and polymer is mentioned: [Pg.284]    [Pg.320]    [Pg.44]    [Pg.182]    [Pg.244]    [Pg.237]    [Pg.1011]    [Pg.1]    [Pg.397]    [Pg.903]    [Pg.903]    [Pg.905]    [Pg.930]    [Pg.936]   


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