Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Pure £-bands

Frontal analysis is a preparative method, used primarily for the separation of one readily eluted component from the other, more tightly held components. The technique is performed by the continuous addition of a sample mixture onto the column. Initially, the component of interest, that is, the component with the least affinity for the stationary phase, will pass through the column while the other sample components are retained to various degrees by the stationary phase. As a result of the continuous sample application, the concentration of bound components steadily builds up at the head of the column. When the column capacity for any given component is exceeded, that component also passes through the column. Therefore, the first component is eluted from the column initially as a pure band and subsequently as a mixture with the next components to be eluted. [Pg.7]

In the final stage of the development of an isotachic train, we obtain n plateaus and as many shock waves one plateau and one shock wave for each pure band y. Since only component / is present in the /th band, and all the other components are missing from that band ... [Pg.457]

In isotachophoresis, electrical detection is most commonly used, although thermal and UV-absorption detection are also used(3). For capillary zone electrophoresis, UV-absorption and fluorescence detection have proven most useful so far. The principles behind the optical detection modes are fairly obvious. However, the electrical and thermal detectors deserve further explanation. As described earlier, in isotachophoresis, each zone is an individual "pure" band of sample ions. The zones travel in order of decreasing mobility. To compensate for each successive... [Pg.13]

Conceptually, the formation of the energy bands is most easily described within the ASA, the atomic-spheres approximation. [4,30,73] A pure band of character (, is the angular momentum), pure in the sense that hybridization is omitted, extends over the energy range Eb () to Ea ) where the logarithmic derivative... [Pg.887]

The fact that the profile for the end of the second component is the same as the profile of a pure band of that compound... [Pg.195]

Another way to see these features is to sketch the MOs that the computer program reports for various k values. These are shown for k = Q,jt /am Fig. 15-14. It is obvious that the lowest band is all 2s at A = 0 and all diik = 7T/a, whereas the highest band is exactly the reverse. The bands have switched character. The pure 2s band we were discussing, that should have gone to very high energy, is represented by a dashed line in Fig. 15-14, and the pure band by another, and these dashed lines do just what we argued they should. [Pg.545]

O Shea and Santry.< > The results, as expected, are very similar, considering the slight difference in geometrical parameters. We note that for overlapping bands in our methodology, the aln nature of a given band may change as k varies, and resolution into pure bands is necessary for direct comparison with their calculations. This is readily accomplished by inspection of the matrices C(k). [Pg.99]

Fig. 3 An illustration of the transport mechanisms described in Sect. 2 for the one dimensional model of Eq. (1). The continuous line represents the density profile of the charge carrier at a given time and the lattice is idealized as an array of diatomic molecules whose bond distance uj can be modulated by the presence of the charge. In pure band transport (a) the carrier travels as a delocahzed wavepacket without deforming the underlying lattice. In polaronic band transport (b), the carrier and a deformation of the lattice form a quasiparticle that behaves as a heavier (and slower) charge carrier. In pure hopping (c), the charge is localized in one site and hops with a given rate to the neighboring sites. The intermediate case between (a) and (b) is studied by large polaion theories, while the transition between (b) and (c) is studied by smaU polaron theories... Fig. 3 An illustration of the transport mechanisms described in Sect. 2 for the one dimensional model of Eq. (1). The continuous line represents the density profile of the charge carrier at a given time and the lattice is idealized as an array of diatomic molecules whose bond distance uj can be modulated by the presence of the charge. In pure band transport (a) the carrier travels as a delocahzed wavepacket without deforming the underlying lattice. In polaronic band transport (b), the carrier and a deformation of the lattice form a quasiparticle that behaves as a heavier (and slower) charge carrier. In pure hopping (c), the charge is localized in one site and hops with a given rate to the neighboring sites. The intermediate case between (a) and (b) is studied by large polaion theories, while the transition between (b) and (c) is studied by smaU polaron theories...
PPha, pyridine) organic groups (olefines, aromatic derivatives) and also form other derivatives, e.g. halides, hydrides, sulphides, metal cluster compounds Compounds containing clusters of metal atoms linked together by covalent (or co-ordinate) bands, metaldehyde, (C2H40) ( = 4 or 6). A solid crystalline substance, sublimes without melting at I12 1I5" C stable when pure it is readily formed when elhanal is left in the presence of a catalyst at low temperatures, but has unpredictable stability and will revert to the monomer, ft is used for slug control and as a fuel. [Pg.257]

A recent study of the vibrational-to-vibrational (V-V) energy transfer between highly-excited oxygen molecules and ozone combines laser-flash photolysis and chemical activation with detection by time-resolved LIF [ ]. Partial laser-flash photolysis at 532 mn of pure ozone in the Chappuis band produces translationally-... [Pg.2139]

The former exhibits absorption tjrpical of an isolated keto group, whereas the latter shows a high intensity -band associated with the conjugated system HO—C=C—C=0. The proportions of the two forms under various conditions are readily determined from the ultraviolet spectra. The ultraviolet spectra in various solvents are shown in Fig. A, 7, 2. Since the absorption of the keto form is negligible, the percentage of enol present is 100(em/e ), where e is the observed extinction at 245 mp. and that of the pure enol. It was shown that in alcoholic solution is 1900 and the percentage of enol is 12. Thus e is ca. 16000, and use of this value permits the approximate evaluation of the enol content in different solvents. The results are collected in Table XII. [Pg.1148]

A typical absorption curve for vitreous siUca containing metallic impurities after x-ray irradiation is shown in Eigure 12. As shown, the primary absorption centers are at 550, 300, and between 220 and 215 nm. The 550-nm band results from a center consisting of an interstitial alkah cation associated with a network substituent of lower valency than siUcon, eg, aluminum (205). Only alkaUes contribute to the coloration at 550 nm. Lithium is more effective than sodium, and sodium more effective than potassium. Pure siUca doped with aluminum alone shows virtually no coloration after irradiation. The intensity of the band is deterrnined by the component that is present in lower concentration. The presence of hydrogen does not appear to contribute to the 550-nm color-center production (209). [Pg.510]

Both anatase and mtile are broad band gap semiconductors iu which a fiUed valence band, derived from the O 2p orbitals, is separated from an empty conduction band, derived from the Ti >d orbitals, by a band gap of ca 3 eV. Consequendy the electrical conductivity depends critically on the presence of impurities and defects such as oxygen vacancies (7). For very pure thin films, prepared by vacuum evaporation of titanium metal and then oxidation, conductivities of 10 S/cm have been reported. For both siugle-crystal and ceramic samples, the electrical conductivity depends on both the state of reduction of the and on dopant levels. At 300 K, a maximum conductivity of 1 S/cm has been reported at an oxygen deficiency of... [Pg.121]

Ordinarily, the energy gap (Eg) between the filled and empty bands is appreciably greater than kT. The concentration of conduction electrons n in the pure stoichiometric material is equal to the concentration of holes p and is given by... [Pg.357]


See other pages where Pure £-bands is mentioned: [Pg.566]    [Pg.91]    [Pg.371]    [Pg.362]    [Pg.2]    [Pg.887]    [Pg.41]    [Pg.302]    [Pg.28]    [Pg.40]    [Pg.544]    [Pg.566]    [Pg.91]    [Pg.371]    [Pg.362]    [Pg.2]    [Pg.887]    [Pg.41]    [Pg.302]    [Pg.28]    [Pg.40]    [Pg.544]    [Pg.2212]    [Pg.2223]    [Pg.2449]    [Pg.48]    [Pg.1136]    [Pg.1144]    [Pg.182]    [Pg.194]    [Pg.629]    [Pg.148]    [Pg.158]    [Pg.236]    [Pg.116]    [Pg.197]    [Pg.200]    [Pg.122]    [Pg.291]    [Pg.446]    [Pg.507]    [Pg.384]    [Pg.64]    [Pg.358]    [Pg.429]    [Pg.105]    [Pg.417]   
See also in sourсe #XX -- [ Pg.20 ]




SEARCH



Extraction of Pure Polymer Additives from Separated Adsorbent Bands

Pure crystals band structure

Pure crystals excitation band

© 2024 chempedia.info