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Isotope exchange from equilibrium

A potential limitation encountered when one seeks to characterize the kinetic binding order of certain rapid equilibrium enzyme-catalyzed reactions containing specific abortive complexes. Frieden pointed out that initial rate kinetics alone were limited in the ability to distinguish a rapid equilibrium random Bi Bi mechanism from a rapid equilibrium ordered Bi Bi mechanism if the ordered mechanism could also form the EB and EP abortive complexes. Isotope exchange at equilibrium experiments would also be ineffective. However, such a dilemma would be a problem only for those rapid equilibrium enzymes having fccat values less than 30-50 sec h For those rapid equilibrium systems in which kcat is small, Frieden s dilemma necessitates the use of procedures other than standard initial rate kinetics. [Pg.298]

Since negative thermal ion mass spectrometry (N-TIMS) for rhenium/osmium dating (see O Sect. 17.18) was developed about 1990, not too much work has been published. This is probably due to the high rhenium blanks from the current generation of clean platinum filaments and to problems in achieving isotopic exchange and equilibrium between sample and spike for osmium. Another drawback is the non-homogeneity of samples. Because of this, rhenium and osmium concentrations may vary hy up to 40% in the same sample. [Pg.777]

Kaplan and Thornton (1967) used three different sets of vibrational frequencies to estimate the zero-point energies of the reactants and products of the equilibrium, which provided three different isotope exchange equilibrium constants 1-163, 1-311 and 1-050. The value 1-311 is considered to be most reasonable, whereas the others are rejected as unrealistic for the case in hand. Calculations using the complete theory led to values that varied from 1-086 to 1-774 for different sets of valence-force constants for the compounds involved. [Pg.20]

McMillan has reviewed the chemistry of Ag(II) and Ag(IlI). Paramagnetism and electron spin resonance studies confirm the presence of Ag(ll) (as opposed to equimolar Ag(I)+Ag(III)). The colours of Ag(II) solutions in various mineral acids indicate the existence of complexes, the oxidising power of which is apparent from their decomposition even at 0 °C, although high acidity promotes stability. Rapid isotope exchange between Ag(I) and Ag(n) is considered to result from the equilibrium... [Pg.354]

Lee and Bethke (1996) presented an alternative technique, also based on mass balance equations, in which the reaction modeler can segregate minerals from isotopic exchange. By segregating the minerals, the model traces the effects of the isotope fractionation that would result from dissolution and precipitation reactions alone. Not unexpectedly, segregated models differ broadly in their results from reaction models that assume isotopic equilibrium. [Pg.270]

Fig. 19.2. Isotopic composition (bold lines) of dolomite formed by reaction between a limestone and migrating groundwater, assuming that minerals maintain isotopic equilibrium over the simulation. Fine lines show results of simulation holding minerals segregated from isotopic exchange, as already presented (Fig. 19.1). Fig. 19.2. Isotopic composition (bold lines) of dolomite formed by reaction between a limestone and migrating groundwater, assuming that minerals maintain isotopic equilibrium over the simulation. Fine lines show results of simulation holding minerals segregated from isotopic exchange, as already presented (Fig. 19.1).
How would the results differ if we had assumed isotopic equilibrium among minerals instead of holding them segregated from isotopic exchange To find out, we enter the commands... [Pg.282]

This latter equilibrium is called an isotopic exchange equilibrium. Its equilibrium constant in terms of partition functions is from Equation 4.64... [Pg.89]

At all but very high temperatures it is necessary to employ the complete equation because the vibrational frequencies for all these molecules are quite high. (Notice at room temperature u(H2) 21, and u(HI) 11). Harmonic oscillator rigid rotor calculated equilibrium constants are shown in Fig. 4.4. As expected the low temperature limiting value, while bounded, is significantly different from unity. At extremely high temperature Equation 4.95 applies and the isotope exchange constant is... [Pg.116]

The products of Rayleigh fractionation are effectively isolated from isotopic exchange with the rest of the system immediately upon formation. If the process occurs slowly, such that each increment of product B forms in isotopic equilibrium with the reactant A prior to isolation of B from the system, then would be an equilibrium isotope fractionation factor. However, if the process of formation of B is rapid, incremental formation of B may be out of isotopic equilibrium withH. In this case, would be a kinetic isotope fractionation factor, which may be a function of reaction rates or other system-specihc conditions. [Pg.14]

Figure 8. Example of apparent closed-system equilibrium fractionation, where Mo in solution is sorbed to Mn oxides (Barling and Anbar 2004). The 6 Mo values of the Mo remaining in solution during sorption follow die linear trends that are consistent widi closed-system equilibrium fractionation where isotopic equilibrium is continuously maintained between Mo in solution and diat sorbed to die Mn oxides. Three aqueous-solid pairs (shown widi tie lines) are consistent with this interpretation. The isotopic data cannot be ejqilained dirough a Rayleigh process, where die product of die reaction (sorbed Mo) is isolated from isotopic exchange widi aqueous Mo. Figure 8. Example of apparent closed-system equilibrium fractionation, where Mo in solution is sorbed to Mn oxides (Barling and Anbar 2004). The 6 Mo values of the Mo remaining in solution during sorption follow die linear trends that are consistent widi closed-system equilibrium fractionation where isotopic equilibrium is continuously maintained between Mo in solution and diat sorbed to die Mn oxides. Three aqueous-solid pairs (shown widi tie lines) are consistent with this interpretation. The isotopic data cannot be ejqilained dirough a Rayleigh process, where die product of die reaction (sorbed Mo) is isolated from isotopic exchange widi aqueous Mo.
Figure 11. Determination of ferrous-ferric isotope exchange kinetics in dilute aqueous solutions using Fe-enriched tracer solutions. Measured 5 Fe values for ferrous (squares) and ferric (circles) Fe in solution versus time. Initial 5 Fe values for Fe(II), 0%o and Fe(III),q 331%o. The rapid convergence in Fe/ Fe ratios for the ferric and ferrous species indicates that isotopic equilibrium is attained within minutes. Adapted from Welch et al. (2003). Figure 11. Determination of ferrous-ferric isotope exchange kinetics in dilute aqueous solutions using Fe-enriched tracer solutions. Measured 5 Fe values for ferrous (squares) and ferric (circles) Fe in solution versus time. Initial 5 Fe values for Fe(II), 0%o and Fe(III),q 331%o. The rapid convergence in Fe/ Fe ratios for the ferric and ferrous species indicates that isotopic equilibrium is attained within minutes. Adapted from Welch et al. (2003).
Kinetic fractionations can occur when there is incomplete isotopic exchange between the different phases present in a system. A thorough introduction to kinetic stable isotope fractionation theory is unfortunately beyond the scope of the present review. Flowever, it is useful to include a brief discussion of some basic aspects, particularly in comparison to equilibrium fractionation theory. A simple example of kinetic fractionation is the evaporation of a liquid water droplet into a vacuum, in this example FljO molecules entering the gas phase are physically removed from the vicinity of the droplet, so there is no chance for isotopic equilibration between vapor-phase molecules and the residual liquid. Isotopic fractionation in this case is determined by a one-way reaction path, and will not, in general, be the same as the fractionation in a system where vapor-phase molecules are able to equilibrate and exchange with the liquid. In other reactions, isotopic exchange is limited by an energy barrier—an... [Pg.92]

Figure 8. Results of Mo adsoqjtion experiments of Barling and Anbar (2004). Mo-bearing solutions were exposed to synthetic Mn oxides (5-Mn02) for 2-96 hours at pH 6.5-8.5. Residual Mo in solution ( ) was measured for all experiments. Mo adsorbed to oxide particle surfaces ( ) was either measured or inferred from mass balance. Dissolved Mo was systematically heavier than adsorbed Mo with a fractionation factor of 1.0018 0.0005. The data are consistent with closed system equilibrium, in which isotopes exchange continuously between surface and solution, but incompatible with an irreversible, Rayleigh-type process. Figure modified after Barling and Anbar (2004). Figure 8. Results of Mo adsoqjtion experiments of Barling and Anbar (2004). Mo-bearing solutions were exposed to synthetic Mn oxides (5-Mn02) for 2-96 hours at pH 6.5-8.5. Residual Mo in solution ( ) was measured for all experiments. Mo adsorbed to oxide particle surfaces ( ) was either measured or inferred from mass balance. Dissolved Mo was systematically heavier than adsorbed Mo with a fractionation factor of 1.0018 0.0005. The data are consistent with closed system equilibrium, in which isotopes exchange continuously between surface and solution, but incompatible with an irreversible, Rayleigh-type process. Figure modified after Barling and Anbar (2004).
Fig. 1.7 Schematic representation of the three-isotope exchange method. Natural samples plotted on the primary mass fractionation hne (PF). Initial isotopic composition are mineral (Mo) and water (Wo) which is well removed from equilibrium with Mq in 8 0, but very close to equUibrium with Mo in 5 0. Complete isotopic equihbrium is defined by a secondary mass fractionation hne (SF) parallel to PF and passing through the bulk isotopic composition of the mineral plus water system. Isotopic compositions of partially equilibrated samples are Mf and Wf and completely equilibrated samples are Mg and Wg. Values for Me and W. can be determined by extrapolation from the measured values of M , Mf, Wo, and Wf (after Matthews et al. 1983a... Fig. 1.7 Schematic representation of the three-isotope exchange method. Natural samples plotted on the primary mass fractionation hne (PF). Initial isotopic composition are mineral (Mo) and water (Wo) which is well removed from equilibrium with Mq in 8 0, but very close to equUibrium with Mo in 5 0. Complete isotopic equihbrium is defined by a secondary mass fractionation hne (SF) parallel to PF and passing through the bulk isotopic composition of the mineral plus water system. Isotopic compositions of partially equilibrated samples are Mf and Wf and completely equilibrated samples are Mg and Wg. Values for Me and W. can be determined by extrapolation from the measured values of M , Mf, Wo, and Wf (after Matthews et al. 1983a...
Selected entries from Methods in Enzymology [vol, page(s)] Equilibrium isotope exchange study of kinetic mechanism, 249, 466 site-directed mutagenesis of Escherichia coli enzyme, 249, 93 positional isotope exchange studies, 249, 423 product inhibition studies of three substrates three products reactions, 249, 207-208. [Pg.36]


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See also in sourсe #XX -- [ Pg.344 ]




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