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Line spectra types

Another spectral change was found w hen a cast film of C AzoCgN+Br was annealed and then moistened (Figure 13). The type I spectrum of the as-cast film changed to the type V spectrum (the broken-line spectrum in Figure 13) after heating above its phase transition (115°C[22]), and then immediately shifted to the type III spectrum within 30 sec in a 75% humidity condition at room temperature. The type III state seemed to be another metastable state in the annealed film because the moisture induced isothermal transition from the type III to the type I required a long period (e.g. 13 hours even at 75% humidity). [Pg.63]

Figure 13. Spectral change of the annealed film (C6AzoC8N+) by moisture treatment. The broken line spectrum of the annealed film was stable in a dry condition but immediately shifted to the type III spectrum within 30 sec in a humid atmosphere. Figure 13. Spectral change of the annealed film (C6AzoC8N+) by moisture treatment. The broken line spectrum of the annealed film was stable in a dry condition but immediately shifted to the type III spectrum within 30 sec in a humid atmosphere.
Hi) Line Spectra Line spectra are usually encountered when the light emitting substance i.e., the radiating species are separate atomic entities (particles) which are distinctly separated from one another, as in gas. Therefore, it is invariably known as atomic spectrum . As the line spectrum depends solely upon the type of an atom, hence it enjoys the status of a predominant type of emission spectroscopy. [Pg.358]

H Oh = 0.5 mT, 4H) suggests an intermediate with Civ symmetry (Fig. 6.12, type At temperatures >77 K, anearly isotropic nine-line spectrum (oh = 1-33 mT) was observed, supporting a dynamic JT effect averaging all eight nuclei. [Pg.224]

The other copper-only binuclear centre to be considered is the CuA or purple copper complex. It is part of the terminal oxidase in mitochondrial respiration, cytochrome c oxidase (COX). Its EPR signature, a seven-line spectrum, has since long been known to be different from the classes type 1 to 3 and arises from two copper ions in a 1.5 valence (or mixed valence) state, first proposed from EPR-analysis of a similar center in nitrous oxide (N20) reductase. There is a close correspondence between the blue and purple states of copper since each of the two copper ions in CuA can be considered as being structurally related to the mononuclear blue site coordination. [Pg.128]

Phosphors doped with rare-earth elements show two types of CTL spectrum, namely emission from the excited species and recombination radiation, simultaneously. Figure 21 shows the CTL spectrum from the TL-phosphor BaS04 Eu in air containing ethanol vapor. The emission band with fine spectrum components at 420 nm is attributed to the excited HCHO. The line spectrum components peaking at 580 and 615 nm are attributed to the electronic transitions within Eu3+ ions. [Pg.117]

Modern atomic theory received a shot in the arm when it was recognized that the individual atom has light absorption and emission spectra occurring at narrow lines of the spectrum at specific wavelengths, as opposed to the broad bands typical of the polyatomic molecules and compounds. Since the line spectrum of each element is characteristic of that element, atomic spectroscopy can be used for precise elementary analysis of many types of chemically simple and complex materials. These studies make use of the wave character of light, as well as light s particle character. [Pg.112]

Types of absorption spectra line spectrum and broadband spectrum. [Pg.504]

The carbon atoms in Ceo are equivalent, and as expected only a single line is observed 5142.7 ppm (CeDe). C70 has Dih symmetry and as there are five distinct carbon atom environments, a five-line spectrum is observed 5150.1, 147.5, 146.8, 144.8, and 130.3 ppm (CeDe) of intensity ratio 10 20 10 20 10 (Figure 15). The initial assignments based on chemical intuition have been subsequently confirmed by 2D C NMR. The upheld line (5130.9 ppm) corresponds to the 10 graphitic atoms around the waist (type e), that he at the intersection of three six-membered rings. [Pg.613]

A similar atom type partition is found for C76. This molecule has D2 synunetry and the expected 19-line spectrum is observed. The four upheld lines (5 < 137.1 ppm) are assigned to the 16 (4 x 4 atoms) graphitic carbons, whereas the remaining 60 carbons (15 x4 atoms, 5 > 141.3 ppm) make up the 12 five-membered rings. Some other higher fiillerenes have been successfidly characterized as mixtures of isomers. Thus for C78, five isomers are possible, but only three have been characterized by C NMR C2v (21 lines), C (21 lines), and D3 (13 lines). For Cg2, nine isomers are possible and three (possibly with traces of a fourth) have been seen, at least one C2 (41 lines), C2 (17 lines), and 3 (12 lines). For Cg4, 24 isomers are possible, but only two have been seen, D2 (21 lines) and D2d (10 lines). [Pg.613]

The mixture of molecular ion and fragments is accelerated to specific velocities using an electric field and then separated on the basis of their different masses by deflection in a magnetic or electrostatic field. Only the cations are detected and a mass spectrum is a plot of mass-to-charge ratio (w/z) on the x-axis against the number of ions (relative abundance, RA, %) on the y-axis. A schematic of the components of a mass spectrometer is shown in Fig. 30.2 and an example of a line-graph-type mass spectrum in Fig. 30.3. [Pg.200]

Fig. 9. CD spectra of the wild type E. coli LamB synthetic signal peptide in phospholipid monolayers. The experiment was carried out as described in Figs. 7 and 8. The solid line spectrum was obtained for films spread at pressures below the peptide s critical pressures of insertion, and the broken line spectrum for films spread above the peptide s critical pressure of insertion. Hence, the former represents inserted plus adsorbed peptide, and the latter is from adsorbed peptide only. Experimental details are reported in Briggs et al. (1986). Copyright 1986 by the American Association for the Advancement of Science. Fig. 9. CD spectra of the wild type E. coli LamB synthetic signal peptide in phospholipid monolayers. The experiment was carried out as described in Figs. 7 and 8. The solid line spectrum was obtained for films spread at pressures below the peptide s critical pressures of insertion, and the broken line spectrum for films spread above the peptide s critical pressure of insertion. Hence, the former represents inserted plus adsorbed peptide, and the latter is from adsorbed peptide only. Experimental details are reported in Briggs et al. (1986). Copyright 1986 by the American Association for the Advancement of Science.

See other pages where Line spectra types is mentioned: [Pg.54]    [Pg.118]    [Pg.71]    [Pg.75]    [Pg.64]    [Pg.419]    [Pg.267]    [Pg.18]    [Pg.124]    [Pg.264]    [Pg.410]    [Pg.153]    [Pg.45]    [Pg.147]    [Pg.393]    [Pg.75]    [Pg.209]    [Pg.209]    [Pg.60]    [Pg.70]    [Pg.337]    [Pg.210]    [Pg.54]    [Pg.28]    [Pg.143]    [Pg.1181]    [Pg.20]    [Pg.346]    [Pg.1005]    [Pg.6087]    [Pg.107]    [Pg.14]    [Pg.208]    [Pg.739]    [Pg.783]    [Pg.3462]    [Pg.142]    [Pg.599]    [Pg.187]    [Pg.734]   
See also in sourсe #XX -- [ Pg.8 ]




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