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Species experimental arrangement used

Figure 8.1.3 Schematic of the experimental arrangement used for continuous-flow 13C NMR experiments employing a pre-column with immobilized paramagnetic species... Figure 8.1.3 Schematic of the experimental arrangement used for continuous-flow 13C NMR experiments employing a pre-column with immobilized paramagnetic species...
Figure 18. Experimental arrangement used in the author s laboratory to measure laser-induced fluorescence signals from flame species... Figure 18. Experimental arrangement used in the author s laboratory to measure laser-induced fluorescence signals from flame species...
When the temperature of the analyzed sample is increased continuously and in a known way, the experimental data on desorption can serve to estimate the apparent values of parameters characteristic for the desorption process. To this end, the most simple Arrhenius model for activated processes is usually used, with obvious modifications due to the planar nature of the desorption process. Sometimes, more refined models accounting for the surface mobility of adsorbed species or other specific points are applied. The Arrhenius model is to a large extent merely formal and involves three effective (apparent) parameters the activation energy of desorption, the preexponential factor, and the order of the rate-determining step in desorption. As will be dealt with in Section II. B, the experimental arrangement is usually such that the primary records reproduce essentially either the desorbed amount or the actual rate of desorption. After due correction, the output readings are converted into a desorption curve which may represent either the dependence of the desorbed amount on the temperature or, preferably, the dependence of the desorption rate on the temperature. In principle, there are two approaches to the treatment of the desorption curves. [Pg.346]

In measuring diffusion in liquids or gases, mixing by convection must be excluded. Several experimental arrangements are described, for example use of a diffusion tube, a diaphragm or a capillary. Measurement of the diffusion coefficient of pH-sensitive species as a function of pH allows conclusions with respect to the size of the species. [Pg.369]

Invention of a simple experimental arrangement lay at the heart of our successful exploitation of aHF, not only in the preparation and characterization of thermodynamically unstable fluorides (Chap. 7) but also (Chap. 8) in the room temperature synthesis of high oxidation-state species (such as [Ag F4] and [Au Fe]") using photodissociated fluorine. Translucent FEP Teflon polymer has made this chemistry possible, since it is not only easily formed into suitable containers for aHF, but it is transparent to the light necessary to the photodissociation of F2. It also has remarkable kinetic stability towards fluorination. Using such apparatus, it has been... [Pg.625]

A further requirement for measurement of absolute concentrations of excited species in flames is that the volume from which emission is collected be known. The simplest experimental arrangement for flames at atmospheric pressures is to focus the radiation from the flame onto the entrance slit of a spectrograph. Reasonable assumptions can be made about the thickness of the emitting layer, and Ausloos and van Tiggelen have used the arrangement successfully in semi-quantitative determinations of excited OH, NH, NO and NH2 in flames emitting the bands of these species. [Pg.287]

In-situ luminescence measurements have been used to study the semiconductor/ electrolyte interface for many years (e.g. Petermann et al., 1972). Luminescence may result from optical excitation of electron/hole pairs that subsequently combine with the emission of light (photoluminescence). Alternatively, minority carriers injected from redox species in the electrolyte can recombine with majority carriers and give rise to electroluminescence. The review by Kelly et al. (1999) summarises the main features of photoluminescence (PL) and electroluminescence (EL) at semiconductor electrodes. The experimental arrangements for luminescence measurements are relatively straightforward. Suitable detectors include a silicon photodiode placed close to the sample, a conventional photomultiplier or a cooled charge-coupled silicon detector (CCD). The CCD system is used with a grating spectrograph to obtain luminescence spectra. [Pg.700]

More recent results have been obtained using a modified version of the previously reported H cell (see Figure 3 below). Two potentiostats are used simultaneously, one to reduce the anthraquinone ligand near the donor organic interface and the other to oxidize the complexed, neutral species near the receiving interface. Such an experimental arrangement has been reported by Saji [20] and is clearly not without its problems. Nevertheless, we have recently shown further cation transport rate enhancements using this approach. Refinements in this approach are still required. [Pg.264]

In the case of infrared absorption, the experimental arrangement consists of using an infrared radiation polarizer placed before the sample under study, conveniently orientated with respect to the crystallographic axes of the latter. Referring to the example of PbCl2 and so forth (see Sec. V.E), if the polarizer is orientated parallel to the z crystallographic axis for example, only the species having the z vector component as its base function will be able to couple with the incident radiation and thus provoke an absorption band. As a consequence, this band will be identified as a Biu(IR z) one. Three such bands are, in principle, observed in the same experimental spectrum, because in the reduction of Fvib for this substance, three Biu(IR z) irreducible representations are obtained [cf. Eq. (8)]. [Pg.410]


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Experimental arrangements

Experimental use

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