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Isotope combinations

Table 8.2 C-O stretch frequency of different isotopic combinations. ... Table 8.2 C-O stretch frequency of different isotopic combinations. ...
Redox gradients in Au systems of the Yilgarn Craton, Western Australia have been mapped across gold lodes and at camp to district scales using C and S isotopes combined with alteration studies. These gradients can be related to the interplay of oxidized and reduced... [Pg.223]

For this reason, these alternative routes for isotope combination with enzyme-substrate and/or enzyme-product complexes ensures that raising the [A]/[Q] or [B]/[P] pair will not depress either the A< Q or the B< P exchanges. Fromm, Silverstein, and Boyer conducted a thorough analysis of the equilibrium exchange kinetic behavior of yeast hexokinase, and the data shown in Fig. 2 indicate that there is a random mechanism of substrate addition and product release. [Pg.388]

An interference check standard is a standard solution used to verify an accurate analyte response in the presence of possible interferences from other analytes present in the samples. For methods that have known interference problems arising from the matrix or that are inherent in the method, such as ICP-AES (spectral interference lines) and ICP-MS (isotope combinations with similar masses to analyte), these solutions are used in the batch. The interference check standard must be matrix matched to acid content of the samples. Acceptance criteria are set—for example, the magnitude of uncorrected background and spectral interference must not be greater than a stated value. [Pg.134]

An ion containing a less abundant combination of isotopes, also included under P.I.D., is not classified separately because identification is usually more simple from the more abundant isotopic combination. The mass number and relative abundance of isotopic ions can be calculated from the accompanying table. It might be argued that classification of these could be useful where the more abundant isotopic combination is obscured by another ion of nominally identical mass. This, however, will be an unusual circumstance and can be overcome by careful use of the table or by the use of exact empirical structure determination through high resolution techniques. [Pg.4]

In closing the section on non-Hermitean approaches to continuum processes in atomic and molecular physics, we will also mention accurate examinations on resonance parameters in molecular predissociation displaying unexpected resonance overlapping [46,89]. The phenomenon of predissociation by rotation in HgH was analyzed via an isotopically combined potential due to Stwalley [120]. The potential, i.e., a relatively shallow energy curve with a nonzero /-value giving rise to a rotational barrier, supported novel metastable states above the dissociation limit. The Weyl s method was able to resolve the closely lying vibrational states v = 3 and v = 4 for the rotational quantum number K = 9. [Pg.71]

Fig. 12. Specular reflectivity for 10-3 M 60/40 SDS/C12E6/D20 onto bare silica ( ) and polyDMDAAC coated silica (A), and (red) for the isotopic combination h-SDS/h-Ci2E6, and (blue) h-SDS/d-C12E6. The solid lines are model calculations. Fig. 12. Specular reflectivity for 10-3 M 60/40 SDS/C12E6/D20 onto bare silica ( ) and polyDMDAAC coated silica (A), and (red) for the isotopic combination h-SDS/h-Ci2E6, and (blue) h-SDS/d-C12E6. The solid lines are model calculations.
Water is composed of hydrogen and oxygen, so it occurs with different isotopic combinations in its molecules. Most common and of interest to hydrochemists are 2 lfiO (common), HD ieO (rare), and lsO (rare). The water molecules may be divided into light molecules ( ieO) and heavy water molecules ( IID ieO and H2 1sO). [Pg.181]

Each observed isotopic peak in spectrum c in Figure 6.6 is also composed of several isotope combinations. For example, the peak marked by an arrow in panel c is shown at high resolution in panel d, where two main peaks appear. According to the observed accurate masses, the first one contains one 34S associated with two 13C, and the second contains four 13C atoms. Indeed the accurate mass of 34S is 33.967080, that of 32S 31.972070, and that of 13C 13.003 355. Thus compared with a molecule containing only the main isotopes of the elements, the shift in mass due to four 13C is 4 x (13.003 355- 12.000000) = 4.0134 u. The shift due to two 13C and one 34S is 2 x (13.003 355 - 12.000 000) + 1 x (33.967 080 - 31.972 070) = 4.0034. [Pg.250]

Useful isotope combinations in mass spectrometry. Isotopes of other atoms that are possibly associated must always be taken into account, as is shown in the framed section. [Pg.252]

Tp = tris(pyrazolyl)borate derivative, L = bispyridine (X = NO) or bisphenolate (X = O) bridging ligands [68]. Because of the presence of only 25.5 % as hyperfine coupling-active nuclei Mo ( Mo with 15.9 % and Mo with 9.6 %, both with I = 5/2), the delocalization is evident from the approximately halved hyperfine coupling constants (as compared with mononuclear Mo species) and from the relative ESR intensities of lines corresponding to molecules with Mo- Mo, Mo-Mo and Mo-Mo isotope combinations [67, 68]. [Pg.1653]

Fig. 6.18. High-resolution spectrum (see Table 6.16) of IT7 (S+) and lTs (S+) in natSi at LHeT showing components associated with different SSi4 isotopic combinations. The FWHMs of 0(rV) and of 0(rg) are 22 and 30peV (0.18 and 0.24cm-1), respectively. The features attributed to 28Si229Si30Si are indicated by arrows [206]. Copyright 2004 by the American Physical Society... Fig. 6.18. High-resolution spectrum (see Table 6.16) of IT7 (S+) and lTs (S+) in natSi at LHeT showing components associated with different SSi4 isotopic combinations. The FWHMs of 0(rV) and of 0(rg) are 22 and 30peV (0.18 and 0.24cm-1), respectively. The features attributed to 28Si229Si30Si are indicated by arrows [206]. Copyright 2004 by the American Physical Society...
Fig. 6.19. Peak fitting of the 11 7 (Se+) profile with Si and Se ISs in natSi obtained by summing the intensities of the 18 strongest SeSi4 isotopic combinations and fitting the peak absorption and energy of the 80Se28Si4 component to 3.28 cm-1 and 427.346 meV [206], Copyright 2004 by the American Physical Society... Fig. 6.19. Peak fitting of the 11 7 (Se+) profile with Si and Se ISs in natSi obtained by summing the intensities of the 18 strongest SeSi4 isotopic combinations and fitting the peak absorption and energy of the 80Se28Si4 component to 3.28 cm-1 and 427.346 meV [206], Copyright 2004 by the American Physical Society...
Isotopic variations of H + H2, obtained by replacing hydrogens by deuteriums, were considered (Wu et al., 1973a) within a different computational scheme (Johnson, 1972) and, in connection with threshold behaviours and resonances for varying isotopic combinations. No significant reaction probabilities were found for total energies below the static barrier potential V s). One-dimensional barriers provided reasonable probabilities only... [Pg.21]

The dashed lines represent the rate constants obtained by transition state theory. The two (close) sets of data for the mixed isotope combinations HD and DH reflect the asymmetry of the barrier. [Pg.933]

Figure 3 is the mass spectrum of the mixture containing 80 mole % MoW(0200(0113)3)4 and 20 mole % Mo2(0200(0113)3)4. The parent ion peaks for the M02 species are centered at 596 amu, those for the MoW species at 683 amu. For the dimolybdenum species, the parent ion set is in good agreement with that expected according to Hochberg et ah (19), and the parent ion set for the MoW species agrees with the expected isotope combinations. However, the relative intensities of the two sets are not an accurate reflection of the composition of the mixture. [Pg.329]


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