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Special Initiation Techniques

As the considerations of Section 3.4.1 demonstrate, an important requirement for either pulsed or cw electronic transition chemical laser operation is the achievement of large metal atom or free-radical concentrations. Moreover, these reagent concentrations must be made available in a manner that ensures that the chemical pumping rate of the upper laser level is large enough compared with the rates of the competing processes of collisional quenching and radiative, decay that an upper level population is created sufficient to exceed laser threshold requirements. [Pg.261]

Experiments directed toward cw chemical laser operation require electrical, thermal, or preferably chemical sources of atoms or radicals. A novel approach under study by Benson, et is the use of a ternary flame [Pg.262]

Another technique of interest has been developed by Friichtenicht and co-workers and applied by Zare et They have made use of a laser-induced vaporization technique for the rapid vaporization and dispersal of a metal into a surrounding oxidizing gas. This method accomplishes the same [Pg.262]

A1 -t- F2 AIF + F reactions, (b) A more-detailed version of the central portion of the apparatus. [Pg.263]


These results are quite interesting. The initial stages of Al deposition result in nanosized deposits. Indeed, from the STM studies we recently succeeded in making bulk deposits of nanosized Al with special bath compositions and special electrochemical techniques [10]. Moreover, the preliminary results on tip-induced nanostructuring show that nanosized modifications of electrodes by less noble elements are possible in ionic liquids, thus opening access to new structures that cannot be made in aqueous media. [Pg.307]

The question of the ( -potential value at the electrolyte solution/air interface in the absence of a surfactant in the solution is very important. It can be considered a priori that it is not possible to obtain a foam film without a surfactant. In the consideration of the kinetics of thinning of microscopic horizontal foam films (Section 3.2) a necessary condition, according to Reynolds relation, is the adsorption of a surfactant at both film surfaces. A unique experiment has been performed [186] in which an equilibrium microscopic horizontal foam film (r = 100 pm) was obtained under very special conditions. A quartz measuring cell was employed. The solutions were prepared in quartz vessels which were purified from surface impurities by a specially developed technique. The strong effect of the surfactant on the rate of thinning and the initial film thickness permitted to control the solution purity with respect to surfactant traces. Hence, an equilibrium thick film with initial thickness of about 120 nm was produced (in the ideal case such a film should be obtained right away). Due to the small film size it was possible to produce thick (100 - 80 nm) equilibrium films without a surfactant. In many cases it ruptured when both surfaces of the biconcave drop contacted. Only very precise procedure led to formation of an equilibrium film. [Pg.142]

The problem of lateral modification of HTSC surface layers, and the local electrosynthesis of HTSCs on the surface of patterned substrates including the precursors is very interesting. Such processes can occur, for example, during electrooxidation of metals when the process in its initial stages takes place only on isolated microscopic regions. Thus, Josephon junctions on the surface of Bi-Sn alloys [222] and on ceramic YBCO samples [295,444] were obtained by using electrochemical oxidation without any special local techniques. But it is hard to control such oxidation processes, and sufficient reproducibility cannot be ensured for most systems. Josephson tunnel junctions based on electrochemically synthesized BKBO crystals have been described [445]. [Pg.98]

High pressure, high temperature membrane sealing is an important aspect of the full scale modirle and this hurdle has been taken for laboratory and bench scale [16,28,31,57]. The membranes can be sealed gas-tight to a stainless steel tube by a special joining technique. Experiments will be carried out initially for the so-called passive reactor concept in which a high selective membrane is surrounded by catalyst. [Pg.672]

In addition to the epidermal abnormalities noted above, there is an increase in the number of dermal cells which is probably of secondaiy importance. However, it should be noted that Weddell (W7, W8) using special histochemical techniques has reported an increased production and breakdown of Schwann cells in the psoriatic lesion, and he believes that these changes are of primary importance in stimulating the epidermal lesion. Along similar lines is the suggestion by Pinkus and Mehregan (P7) that the polymorphonuclear leukocytes are of prime importance in stimulating the epidermis and that the dilated capillary in the papilla squirts these leukocytes into the epidermis as an initial event. [Pg.327]

Whatever the precise mechanism is, it has been noted that generally polymerizations of vinyl ethers occur rapidly under electrolytic conditions to give high yields of polymer per Faraday of current passed. However, in most cases, only low-molecular-weight polymers are obtained. Until major breakthroughs are made, electrochemical initiation must be regarded as a rather special, nonroutine technique for the polymerization of vinyl ethers. [Pg.177]

Impedance spectroscopy offers the possibility to study various phenomena. Here we first focus on delamination. In the next section we discuss the study of corrosion initiation. The study of the curing of coatings and special monitoring techniques has been left out of the discussion [7,9,87-91]. [Pg.710]

Figure 2.14. Guinier transmission diffraction patterns using Co K a-radiation. The samples were analyzed after the specific surface area determination. A special embedding technique protected the material from exposure to air, the efficiency of which is demonstrated in the scan of the sample activated at 423 °C. It can be seen that as a consequence of the fracture of the initial magnetite crystallites during reduction, the texture effect in the magnetite diffraction pattern is lost (see scan at 385 °C). Figure 2.14. Guinier transmission diffraction patterns using Co K a-radiation. The samples were analyzed after the specific surface area determination. A special embedding technique protected the material from exposure to air, the efficiency of which is demonstrated in the scan of the sample activated at 423 °C. It can be seen that as a consequence of the fracture of the initial magnetite crystallites during reduction, the texture effect in the magnetite diffraction pattern is lost (see scan at 385 °C).
Specially designed techniques for determination of kfi,i) are based on controlling the radical chain length either by laser single-pulse initiation ... [Pg.47]

Best Synthetic Methods is now 10 years old, is a family of 16 volumes and has been well received by the majority of chemists as a valuable aid in their synthetic endeavours, be they academic or commercial. The focus of the series so far has been on special methods, reagents or techniques. This volume is the first of a new sub-series with a focus on heterocycles and their synthesis. It is amazing the extent to which each heterocyclic type has its own specialized synthetic methodology. Whether the chemist is endeavouring to make a heterocycle by ring synthesis or wishes to introduce specific substituents, it is the intention that this new development will serve their needs in a practical, authoritative, fully illustrative and compact manner. Richard Sundberg is an authority on indole chemistry and it is a pleasure to have such a noted heterocyclist to initiate this venture. [Pg.181]

The AeroSizer, manufactured by Amherst Process Instmments Inc. (Hadley, Massachusetts), is equipped with a special device called the AeroDisperser for ensuring efficient dispersal of the powders to be inspected. The disperser and the measurement instmment are shown schematically in Figure 13. The aerosol particles to be characterized are sucked into the inspection zone which operates at a partial vacuum. As the air leaves the nozzle at near sonic velocities, the particles in the stream are accelerated across an inspection zone where they cross two laser beams. The time of flight between the two laser beams is used to deduce the size of the particles. The instmment is caUbrated with latex particles of known size. A stream of clean air confines the aerosol stream to the measurement zone. This technique is known as hydrodynamic focusing. A computer correlation estabUshes which peak in the second laser inspection matches the initiation of action from the first laser beam. The equipment can measure particles at a rate of 10,000/s. The output from the AeroSizer can either be displayed as a number count or a volume percentage count. [Pg.134]

Developments in experimental and mathematical techniques in the 1970s have initiated an interest in the development of better laboratory reactors for catal5d ic studies. Besides the many publications on new reactors for general or special tasks, quite a few review articles have been published on the general subject of laboratory reactors for catalytic studies. [Pg.5]

Since the first separation of enantiomers by SMB chromatography, described in 1992 [95], the technique has been shown to be a perfect alternative for preparative chiral resolutions [10, 21, 96, 97]. Although the initial investment in the instrumentation is quite high - and often prohibitive for small companies - the savings in solvent consumption and human power, as well as the increase in productivity, result in reduced production costs [21, 94, 98]. Therefore, the technique would be specially suitable when large-scale productions (>100 g) of pure enantiomers are needed. Despite the fact that SMB can produce enantiomers at very high enantiomeric excesses, it is sometimes convenient to couple it with another separation... [Pg.7]


See other pages where Special Initiation Techniques is mentioned: [Pg.261]    [Pg.261]    [Pg.1082]    [Pg.11]    [Pg.258]    [Pg.273]    [Pg.193]    [Pg.905]    [Pg.1250]    [Pg.18]    [Pg.1251]    [Pg.1086]    [Pg.54]    [Pg.275]    [Pg.80]    [Pg.110]    [Pg.64]    [Pg.125]    [Pg.117]    [Pg.58]    [Pg.161]    [Pg.436]    [Pg.398]    [Pg.295]    [Pg.245]    [Pg.327]    [Pg.452]    [Pg.489]    [Pg.1027]    [Pg.176]    [Pg.220]    [Pg.8]    [Pg.556]   


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Initiation techniques

Special Techniques

Specialized Techniques

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