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Liquid mirrors

Little attention has been given to the influence of these transient liquid mirrors and lenses on the amount of stray light reaching the detector. Investigation of this process is strongly recommended, as the Schlieren effect can lead to an increase in detected radiation, hence degrading the linearity of the analytical response curve [13]. [Pg.125]

Under poor mixing conditions (dominance of component A), there are sharp concentration discontinuities instead of a true gradient function along the flowing sample. A myriad of transient liquid mirrors is established within the poorly mixed fluid elements with different concentrations, and hence refractive indices. The incident beam then undergoes attenuation, mainly by reflection, leading to a decrease in the power of transmitted radiation and therefore to an increase in, e.g., absorbance. [Pg.126]

Hardacre et al. [8] were able to show that the general structure of the liquid mirrors that of NaCl quite closely, despite the obvious differences in size and chemistry between Na" and [Cimim]. For example, ion-ion RDFs (Figure 4.2) show a clear oscillatory structure, with the... [Pg.119]

Figure 2. Schematic of the experimental arrangement used for inspection of aluminium plate. Lenses are shown as LI and L2, mirrors as Ml, M2 and M3, and liquid crystal cell as LC... Figure 2. Schematic of the experimental arrangement used for inspection of aluminium plate. Lenses are shown as LI and L2, mirrors as Ml, M2 and M3, and liquid crystal cell as LC...
An important distinction among surfaces and interfaces is whether or not they exliibit mirror synnnetry about a plane nonnal to the surface. This synnnetry is particularly relevant for the case of isotropic surfaces (co-synnnetry), i.e. ones that are equivalent in every azunuthal direction. Those surfaces that fail to exliibit mirror synnnetry may be tenned chiral surfaces. They would be expected, for example, at the boundary of a liquid comprised of chiral molecules. Magnetized surfaces of isotropic media may also exliibit this synnnetry. (For a review of SFIG studies of chiral interfaces, the reader is referred to [68]. ... [Pg.1286]

A schematic diagram of the surface of a liquid of non-chiral (a) and chiral molecules (b) is shown in figure Bl.5.8. Case (a) corresponds to oom-synnnetry (isotropic with a mirror plane) and case (b) to oo-symmetry (isotropic). For the crj/ -synnnetry, the SH signal for the polarization configurations of s-m/s-out and p-m/s-out vanish. From table Bl.5.1. we find, however, that for the co-synnnetry, an extra independent nonlinear susceptibility element, is present for SHG. Because of this extra element, the SH signal for... [Pg.1286]

An orientational order parameter can be defined in tenns of an ensemble average of a suitable orthogonal polynomial. In liquid crystal phases with a mirror plane of symmetry nonnal to the director, orientational ordering is specified. [Pg.2555]

Figure C3.5.11. IR-Raman measurements of vibrational energy flow tlirough acetonitrile in a neat liquid at 300 K, adapted from [41], An ultrashort mid-IR pulse pumps the C-H stretch, which decays in 3 ps. Only 1% of the energy is transferred to the C N stretch, which has an 80 ps lifetime. Most of the energy is transferred to the C-H bend plus about four quanta of C-C=N bend. The daughter C-H bend vibration relaxes by exciting the C-C stretch. The build-up of energy in the C-C=N bend mirrors the build-up of energy in the bath, which continues for about 250 ps after C-H stretch pumping. Figure C3.5.11. IR-Raman measurements of vibrational energy flow tlirough acetonitrile in a neat liquid at 300 K, adapted from [41], An ultrashort mid-IR pulse pumps the C-H stretch, which decays in 3 ps. Only 1% of the energy is transferred to the C N stretch, which has an 80 ps lifetime. Most of the energy is transferred to the C-H bend plus about four quanta of C-C=N bend. The daughter C-H bend vibration relaxes by exciting the C-C stretch. The build-up of energy in the C-C=N bend mirrors the build-up of energy in the bath, which continues for about 250 ps after C-H stretch pumping.
Because diastereomers are not mirror images of each other they can have quite different physical and chemical properties For example the (2R 3R) stereoisomer of 3 ammo 2 butanol is a liquid but the (2R 3S) diastereomer is a crystalline solid... [Pg.302]

Infrared spectroscopy is routinely used for the analysis of samples in the gas, liquid, and solid states. Sample cells are made from materials, such as NaCl and KBr, that are transparent to infrared radiation. Gases are analyzed using a cell with a pathlength of approximately 10 cm. Longer pathlengths are obtained by using mirrors to pass the beam of radiation through the sample several times. [Pg.393]

Spiegel, m. mirror, speculum, refiector polished surface surface (of liquids, fabrics,... [Pg.418]

Palladium and gold Palladium electrodeposition is of special interest for catalysis and for nanotechnology. It has been reported [49] that it can be deposited from basic chloroaluminate liquids, while in the acidic regime the low solubility of PdCl2 and passivation phenomena complicate the deposition. In our experience, however, thick Pd layers are difficult to obtain from basic chloroaluminates. With different melt compositions and special electrochemical techniques at temperatures up to 100 °C we succeeded in depositing mirror-bright and thick nanocrystalline palladium coatings [10]. [Pg.302]

All currents that had to be measured were sent to a central measurement room in which many mirror galvanometers were situated on top of vibration-free columns that were separated from the foundations of the building. One should realize that the many announcements in the early literature of the liquefaction of specific gases pertained to not much more than a mist or a few drops Kamerlingh Onnes planned to make liquid gases by the gallon. A separate hydrogen liquefaction plant was located in a special room with a roof that could be blown off easily. [Pg.686]

In order to compensate for the distortions in the wavefront due to the atmosphere we must introduce a phase correction device into the optical beam. These phase correction devices operate by producing an optical path difference in the beam by varying either the refractive index of the phase corrector (refractive devices) or by introducing a variable geometrical path difference (reflective devices, i.e. deformable mirrors). Almost all AO systems use deformable mirrors, although there has been considerable research about liquid crystal devices in which the refractive index is electrically controlled. [Pg.191]

However, some interconversion reactions take place simultaneously and therefore the composition of the sulfane mixtime is not a mirror image of the composition of the polysulfide solution [103]. The sulfane mixture forms a yellow oily hydrophobic liquid which precipitates from the aqueous phase. At 20 °C it decomposes more or less rapidly to H2S and Sg. [Pg.143]


See other pages where Liquid mirrors is mentioned: [Pg.297]    [Pg.297]    [Pg.44]    [Pg.137]    [Pg.297]    [Pg.123]    [Pg.578]    [Pg.471]    [Pg.305]    [Pg.95]    [Pg.498]    [Pg.297]    [Pg.297]    [Pg.44]    [Pg.137]    [Pg.297]    [Pg.123]    [Pg.578]    [Pg.471]    [Pg.305]    [Pg.95]    [Pg.498]    [Pg.680]    [Pg.682]    [Pg.1032]    [Pg.116]    [Pg.62]    [Pg.1827]    [Pg.174]    [Pg.418]    [Pg.285]    [Pg.949]    [Pg.62]    [Pg.19]    [Pg.50]    [Pg.73]    [Pg.283]    [Pg.419]    [Pg.81]    [Pg.99]    [Pg.285]    [Pg.144]    [Pg.1032]   
See also in sourсe #XX -- [ Pg.137 ]

See also in sourсe #XX -- [ Pg.305 ]




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