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Isotopic mixing

Isotopic composition of He is described either directly by ratio of isotopes ( He/ Hel pj, or by ratio of ( He/ He) p,y ( He/ He) j. These isotopes in groxmd water may have three different sources atmosphe radiogenic and mantle. The atmospheric helium comes with surface water in the amount of no greater than 0.04-10 cm T and with isotopic ratio He/ He of about (1.39 0.01)10 Radiogenic helium forms as a result of decay of, 9 2 U and 9 2 U and has He/ He isotope ratio on the order of (Tolstikhin, 1986). In 1969, Boris Alexandrovich Mamyrin (1919-2007), or Igor Nestorovich Tolstikhin (b.in 1937) and some others discovered that the Earth mantle preserved He from the moment of the planet formation (Mamyrin and Tolstikhin, 1981). This helium was dubbed primordial helium. That is why the isotopic ratio He/ He in the mantle helium turned out much higher than 1.39-10 and is believed to be (1.2 0.3)-10 (Tolstikhin, 1986). [Pg.414]

Then the atmospheric and radiogenic argon content in water may be determined if total volume content of argon is known  [Pg.415]

and C , are volume concentrations of total, atmo-spheric and radiogenic argon in water, respectively. [Pg.415]

If we assume that the content of the atmospheric argon in surface water is relatively stable then its volume in ground water may be used for estimation of relative content of other chemically passive gas components. That is why concentrations of gas components are sometimes normalized as the ratio of their concentrations and the content of air argon. [Pg.415]

Isotopic composition of N. is determined by ratio of isotopes and Most of this nitrogen is concentrated in the atmosphere and has very stable isotopic ratio equal to 272.2. This atmospheric nitrogen is [Pg.415]


For those who are familiar with the statistical mechanical interpretation of entropy, which asserts that at 0 K substances are nonnally restricted to a single quantum state, and hence have zero entropy, it should be pointed out that the conventional thennodynamic zero of entropy is not quite that, since most elements and compounds are mixtures of isotopic species that in principle should separate at 0 K, but of course do not. The thennodynamic entropies reported in tables ignore the entropy of isotopic mixing, and m some cases ignore other complications as well, e.g. ortho- and para-hydrogen. [Pg.371]

The values of S° represent the virtual or thermal entropy of the substance in the standard state at 298.15 K (25°C), omitting contributions from nuclear spins. Isotope mixing effects are also excluded except in the case of the H—system. [Pg.532]

A special case of opposing reactions is the one in which chemical equilibrium has been attained, but not isotopic equilibrium. Isotopic equilibration reactions are termed exchange reactions. They occur with virtually no net driving force i.e., AG 4 is very nearly zero, save for that provided by the entropy of isotopic mixing. [Pg.55]

The effect of solvent upon k2 has been reported , and it was concluded that the activated complex is not sufficiently polar to be called ionic . The oxidations of toluene and triphenylmethane exhibit primary kinetic deuterium isotope effects of 2.4 and ca. 4 respectively. No isotopic mixing occurred during formation of the Etard complex from a mixture of normal and deuterated o-nitrotoluene . The chromyl chloride oxidation of a series of substituted diphenylmethanes revealed that electron-withdrawing substituents slow reaction while electronreleasing groups have the opposite effect, the values ofp andp being —2.28 + 0.08 and —2.20 + 0.07 respectively . ... [Pg.296]

The intensity of the dicarbonyl at 2116cm is considerably reduced as compared to the 90 K deposit, indicating that the amount of metal atoms trapped at point defects is reduced for growth at 60 K. The difference in the nucleation sites is also reflected by the lower thermal stability of the systems, which decompose between 80 and 150 K as compared to 200 to 250 K for the 90 K deposits. With isotope mixing experiments the peak at 2087 cm was assigned to a carbonyl with three or more CO ligands, while the peak at 1999 cm is associated to a monocarbonyl [32]. [Pg.123]

An important group of analytical methods is based on measurements of the change in isotopic ratio when active and non-active isotopes are mixed. In the simplest case, a known amount w1 of labelled analyte of known specific activity at is added to the sample. After isotopic mixing has been established sufficient of the analyte is separated (nor normally 100%) to allow the new specific activity a2 to be measured. Measurements of activity and the amount of the analyte separated are thus required. Subsequently the amount w2 of analyte in the sample may be calculated from equation (10.17). [Pg.468]

Although the pathway of Eq. (1) is now based on much evidence (Section 111) and is unambiguous in the case of at least one bacterium [Pseudomonas stutzeri strain Zobell (f. sp. P. perfectomarina)], there have been alternative hypothesis. One hypothesis, advanced by the Hollocher group (Garber and Hollocher, 1981 St. John and Hollocher, 1977), considered NO as a likely intermediate, but one that remained at least partly enzyme-bound and was not entirely free to diffuse. This view was based on the outcome of certain kinetic and isotope experiments which can be summarized as follows. When denitrifying bacteria were challenged simultaneously with [ N]nitrite and ordinary NO, the cells reduced both compounds concomitantly to N2 (or to N2O in the presence of acetylene which is a specific inhibitor (Balderston et al., 1976 Yoshinari and Knowles, 1976) of nitrous oxide reductase). In the process, little NO was generally detected in the gas phase pool of NO and there was relatively little isotopically mixed N2O formed. That is, most of the N and N reduced to NjO appeared as N2O... [Pg.294]

Fig. 2.17 Portion of a pulsed-laser time-of-flight spectrum showing the formation of doubly charged Mo diatomic cluster ions in pulsed-laser stimulated field evaporation of Mo. From a multinomial expansion analysis, it is concluded that few Mo+ ions are formed. Although there are a total of only 438 ions in the entire spectrum, all the expected 15 mass lines due to an isotope mixing of the 7 Mo isotopes are present. A mass line, even when it contains only three ions such as that of Min = 100, is clearly identifiable. Fig. 2.17 Portion of a pulsed-laser time-of-flight spectrum showing the formation of doubly charged Mo diatomic cluster ions in pulsed-laser stimulated field evaporation of Mo. From a multinomial expansion analysis, it is concluded that few Mo+ ions are formed. Although there are a total of only 438 ions in the entire spectrum, all the expected 15 mass lines due to an isotope mixing of the 7 Mo isotopes are present. A mass line, even when it contains only three ions such as that of Min = 100, is clearly identifiable.
In an outer-sphere electron transfer the actual electron transfer is iso-energetic and takes place in 10 16 s, during which time, by the Franck-Condon principle, the heavier nuclei do not move. Since protons are known to tunnel (Bell et ah, 1956 Bell, 1973 Caldin, 1969 Lewis, 1975) and since the electron is 2000 times lighter than the proton, it is almost certain that in the actual electron transfer the electron tunnels. For instance, in an isotopic mixing experiment (16) the barrier to the reaction (k = 8 m-1 s-1) lies in achieving the... [Pg.97]

In Fig. 7 we have taken a symmetrical reaction where, apart from the isotopic mixing, AG ° = 0. One of the first successes of the Marcus theory was the correlation of rates for such homogeneous reactions with the rates found for the same electron transfer taking place on an electrode (Marcus, 1963). The theory then went on to predict the rates of cross reactions between two different redox couples in terms of the kinetic and thermodynamic properties of the two redox couples. The free energy profile for an unsymmetrical cross reaction such as (17) is shown in Fig. 8. The free energy of activation depends... [Pg.98]

The present chapter is devoted exclusively to an analysis of the problems of isotopically mixed solvents. It will not concern itself, except in passing, with the measurement and interpretation of solvent effects on equilibrium and rate constants due to the isotopic change from pure H20 to pure D20. The aim is to show to what extent measurements of this type are of practical utility, especially as a tool in the investigation of reaction mechanisms. For this reason, the development of theory is mainly directed towards compromise solutions of a complex problem, i.e. solutions which enable the theory to be tested and applied but lay no claim to being theoretically unassailable. The guiding principle has been to cast the formulation in terms of parameters or types of measurement which are either known or at least known to be feasible. [Pg.260]

The rule of the geometric mean (Bigeleisen, 1955) governs isotopic mixing equilibria, such as (4). [Pg.266]

Since we are dealing in all these equations with dimensionless ratios of mole fractions, we may replace mole fractions by molarities (designated by square brackets) or, indeed, any convenient molecular concentration units. The distribution of H and D among isotopically mixed species is then generally given by a Poisson distribution, i.e. we have for the fractional abundance F of a species XDJ)Hni i, (Cadogan et al., 1955 Kresge, 1964) ... [Pg.267]

Early workers in the field of H20-D20 systems recognized that it was possible to define different acidity constants for the isotopic hydrogen ions, that for an isotopically mixed ion it was necessary to distinguish between proton acidity and deuteron acidity and that it... [Pg.277]

Accordingly, the catalytic coefficients of hydrogen ion in the isotopically pure media (ka and kD) are related to the coefficients of HsO+ and D80+ in isotopically mixed media by the equations ... [Pg.291]

As a mechanistic tool in the investigation of acid- or base-catalysed reactions in aqueous solution, the measurements in isotopically mixed solvents are most useful for reactions where a certain amount is already known about the mechanism. In particular, the study of mixed solvents is also a good deal more informative whenever it is possible to measure product isotope effects in addition to rate isotope effects. In such cases (and A-Sb2 reactions spring to mind as a good example) solvent isotope effect studies can add considerably to the detailed picture of a transition state. The phenomena are as yet less suited to the ah initio assignment of reaction mechanism, such as the decision between weak nucleophilic participation of water in an acid-catalysed reaction and an A-l mechanism, when no information beyond the kn-n relation is available. For these reasons it is likely that mechanistic investigation by this method will increasingly be directed towards systems where both rate and product isotope effects are obtainable. [Pg.327]

Product composition from isotopically mixed solvents... [Pg.69]

Evidence from NMR spectra (Kresge and Allred, 1963 Gold, 1963) supports the intuitively attractive idea that only the M30+ unit of M+, in an isotopically mixed solvent, has an isotopic composition significantly different from the water. The isotopic equilibrium constant, l (0-69, Section IIA4), then pertains to the distribution of isotopes between MsO+ and M20. It could be calculated if the frequency distributions (including librations and restricted translations) were known for liquid H20, D20, and H+ and D+ in those solvents. Since only uncertain approximations of typical frequencies are available, an unsophisticated estimate, made by means of equation (62) (Bunton and Shiner, 1961a)... [Pg.87]


See other pages where Isotopic mixing is mentioned: [Pg.2495]    [Pg.170]    [Pg.253]    [Pg.12]    [Pg.139]    [Pg.27]    [Pg.295]    [Pg.324]    [Pg.60]    [Pg.493]    [Pg.104]    [Pg.60]    [Pg.138]    [Pg.140]    [Pg.179]    [Pg.361]    [Pg.364]    [Pg.31]    [Pg.644]    [Pg.260]    [Pg.268]    [Pg.284]    [Pg.295]    [Pg.310]    [Pg.320]    [Pg.104]    [Pg.70]    [Pg.70]    [Pg.89]    [Pg.226]   


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Entropy of isotope mixing

Isotope mixing

Isotopic labeling, mixed

Isotopic mixed crystals

Kinetic Isotope Effects in Mixed Solvents

Macroscopic surface excitons and polaritons in isotopically mixed crystalline solutions

Mixed isotope photoaffinity

Mixed isotope photoaffinity reagents

Mixed isotopic exponents

Mixed-oxide fuel, isotopic composition

Organic matter isotopic mixing models

Using isotope correlation diagrams and epsilon plots to recognize mixing processes

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