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Middle polar phases

B) Hydrophobic phases with distinct polar character (middle polar phases)... [Pg.200]

Figure 6.55 Distortion of TiOg octahedron in the tetragonal BaTiOs (top) and possible orientations of the polar axis when an electric field is applied along the pseudo-cubic (001) direction of BaTi03 (middle). Polar axes are shown by arrows inside each cube. Phase transitions in BaTiOj accompanied by changes in (a) dielectric constant (b) spontaneous polarization (c) heat capacity and (d) lattice dimensions (bottom). Figure 6.55 Distortion of TiOg octahedron in the tetragonal BaTiOs (top) and possible orientations of the polar axis when an electric field is applied along the pseudo-cubic (001) direction of BaTi03 (middle). Polar axes are shown by arrows inside each cube. Phase transitions in BaTiOj accompanied by changes in (a) dielectric constant (b) spontaneous polarization (c) heat capacity and (d) lattice dimensions (bottom).
SB-biphenyl-30 This stationary phase has 30% biphenyl substitu which provides enhanced polarizability when compared to phe substituted stationary phases. It is in the middle polarity range the SFC stationary phases. [Pg.126]

While the sulfuric acid is key nucleation precursor in the low troposphere, its contribution to the polar stratospheric chemistry is a lot more modest. Another strong acid-nitric-plays a major role as the dominant reservoir for ozone destroying odd nitrogen radicals (NOj) in the lower and middle polar stratosphere. Nitric acid is an extremely detrimental component in the polar stratosphere clouds (PSCs), where nitric acid and water are the main constituents, whose presence significantly increases the rate of the ozone depletion by halogen radicals. Gas-phase hydrates of the nitric acid that condense and crystallize in the stratosphere play an important role in the physics and chemistry of polar stratospheric clouds (PSCs) related directly to the ozone depletion in Arctic and Antarctic. [Pg.453]

Figure 8.19 illustrates another example of the versatility of multidimensional OPLC, namely the use of different stationary phases and multiple development ("D) modes in combination with circular and anticircular development and both off-line and on-line detection (37). Two different stationary phases are used in this configuration. The lower plate is square (e.g. 20 cm X 20 cm), while the upper plate (grey in Figure 8.19) is circular with a diameter of, e.g. 10 cm. The sample must be applied on-line to the middle of the upper plate. In the OPLC chamber the plates are covered with a Teflon sheet and pressed together under an overpressure of 5 MPa. As the mobile phase transporting a particular compound reaches the edge of the first plate it must-because of the forced-flow technique-flow over to the second (lower) stationary phase, which is of lower polarity. [Pg.190]

Butanes are chosen as the simplest models for the normal and branched isomers. Both branched and normal isomers contain a C-C bond (2 ) interacting with the terminal C-H bonds (2 and 2 ) (Scheme 26a). The cyclic -aj-a2 -a3 a2- interaction (Scheme 26b) occurs in the polarization of the middle C-C a-bond by the interactions with the antiperiplanar C-H a-bonds. The orbital phase is continuous in the branched isomer and discontinuous in the normal isomer (cf Scheme 4). The branched isomer is more stable. The basic rule of the branching effects on the stability of alkanes is ... [Pg.105]

It is now instructive to ask why the achiral calamitic SmC a (or SmC) is not antiferroelectric. Cladis and Brand propose a possible ferroelectric state of such a phase in which the tails on both sides of the core tilt in the same direction, with the cores along the layer normal. Empirically this type of conformational ferroelectric minimum on the free-energy hypersurface does not exist in known calamitic LCs. Another type of ferroelectric structure deriving from the SmCA is indicated in Figure 8.13. Suppose the calamitic molecules in the phase were able to bend in the middle to a collective free-energy minimum structure with C2v symmetry. In this ferroelectric state the polar axis is in the plane of the page. [Pg.479]

Table VI shows the results of polarized light microscopic observations. Sometimes isotropic regions and the middle phase exist simultaneously. The region of the middle phase is marked by heavy lines. The range of the especially viscous middle phase narrows with transition from two to three oxyethylene groups in the surfactant molecule. Up to 27 %, the system appears optically isotropic. In this concentration range the viscosity can be increased strongly by addition of NaCl, as shown in table VII. Table VI shows the results of polarized light microscopic observations. Sometimes isotropic regions and the middle phase exist simultaneously. The region of the middle phase is marked by heavy lines. The range of the especially viscous middle phase narrows with transition from two to three oxyethylene groups in the surfactant molecule. Up to 27 %, the system appears optically isotropic. In this concentration range the viscosity can be increased strongly by addition of NaCl, as shown in table VII.
Much chemistry, perhaps most chemistry, is carried out not in the gas phase, but in solution. A wide variety of solvents are available to chemists. At one end of the spectrum is water which is both highly polar and highly structured. Water is unique among common solvents in that it is capable of forming hydrogen bonds to both (proton) donors and acceptors. At the other end of the spectrum are hydrocarbons such as decane, and relatively non-polar molecules such as methylene chloride. In the middle are a whole range of solvents such as tetrahydrofuran which differ both in their polarity and in their ability to act either as hydrogen-bond donors or acceptors. [Pg.49]

One interfacial tension (upper left) is considered located between water and the polar parts (unfilled circles) of the surfactant (upper right) and one (middle left) between the nonpolar part (filled circles) of the surfactant and the hydrocarbon (middle right). The different convexities of the O/W interface giving normal micelles, a surfactant phase or an inverse micelle are formally referred to different ratios of these interfacial tensions (bottom of figure) at a plane interface. [Pg.39]

Fig. 2 Polarizing optical micrographs in the B4 phase of bent-core LC. Under crossed polarizers, texture with bluish color is observable (middle). By decrossing polarizers, two brighter and darker domains are observable (right and left). The brightness is interchanged by decrossing polarizers to counter senses [11]... Fig. 2 Polarizing optical micrographs in the B4 phase of bent-core LC. Under crossed polarizers, texture with bluish color is observable (middle). By decrossing polarizers, two brighter and darker domains are observable (right and left). The brightness is interchanged by decrossing polarizers to counter senses [11]...
Figure 7a displays a SFM phase image of a spin-coated S47H10M4382 film that has a disordered surface structure. The ordering effect of the simultaneous solvent vapor annealing and application of a voltage between the electrodes is shown in Fig. 7b. After 6.5 h of treatment the stripe pattern appears highly ordered parallel to the electric field vector. Importantly, during the swelling of the film, the polar middle PHEMA block remains anchored to the substrate. This preserves the self-assembled stripe pattern of the two major PS and PMMA blocks (Fig. 7c). Figure 7a displays a SFM phase image of a spin-coated S47H10M4382 film that has a disordered surface structure. The ordering effect of the simultaneous solvent vapor annealing and application of a voltage between the electrodes is shown in Fig. 7b. After 6.5 h of treatment the stripe pattern appears highly ordered parallel to the electric field vector. Importantly, during the swelling of the film, the polar middle PHEMA block remains anchored to the substrate. This preserves the self-assembled stripe pattern of the two major PS and PMMA blocks (Fig. 7c).
Figure 3.7 Illustration of the selection of phase systems for LC according to eqn.(3.30). A solute with a polarity of 12.5 (middle scale) can be eluted from silica (Ss= 16 top scale) with a non-polar mobile phase (Sm=9 bottom scale) or with a polar solvent in a reversed phase system. The shaded areas indicate the latitude with respect to the selection of the mobile phase. Figure taken from ref. [311]. Reprinted with permission. Figure 3.7 Illustration of the selection of phase systems for LC according to eqn.(3.30). A solute with a polarity of 12.5 (middle scale) can be eluted from silica (Ss= 16 top scale) with a non-polar mobile phase (Sm=9 bottom scale) or with a polar solvent in a reversed phase system. The shaded areas indicate the latitude with respect to the selection of the mobile phase. Figure taken from ref. [311]. Reprinted with permission.

See other pages where Middle polar phases is mentioned: [Pg.94]    [Pg.7]    [Pg.241]    [Pg.1188]    [Pg.1992]    [Pg.519]    [Pg.2562]    [Pg.204]    [Pg.196]    [Pg.472]    [Pg.474]    [Pg.192]    [Pg.90]    [Pg.148]    [Pg.873]    [Pg.113]    [Pg.23]    [Pg.110]    [Pg.120]    [Pg.78]    [Pg.820]    [Pg.82]    [Pg.237]    [Pg.251]    [Pg.65]    [Pg.80]    [Pg.394]    [Pg.395]    [Pg.119]    [Pg.508]    [Pg.509]    [Pg.264]    [Pg.314]    [Pg.10]    [Pg.43]    [Pg.223]   
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Middlings

Polar phase

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