Vibrational analysis of acetate ion molecules and estimation of equilibrium constants for their hydrogen isotopic exchange reactions

1983 ◽  
Vol 87 (14) ◽  
pp. 2526-2535 ◽  
Author(s):  
Masato Kakihana ◽  
Masahiro Kotaka ◽  
Makoto Okamoto
Author(s):  
Robert E. Criss

Equilibrium isotopic fractionations are best understood in terms of reactions that involve the transfer of isotopes between two phases or molecular species that have a common element (M). These isotopic exchange reactions may be written in one of several standard forms, such as . . . aAM*b + cBMd = aAMb + cBM*d (2.1) . . . where AMb and BMd represent the chemical formulas of the phases or species, AM*b and BM*d represent the same phases or species in which the trace isotope has replaced some or all of the atoms of element M, and a, b, c, and d are stoichiometric coefficients. In the case where all of the molecules are homogeneous, that is, where AMb and BMd are composed solely of the common isotope of M, and where AM*b and BM*d are phases or species in which the trace isotope M* has replaced all atoms of element M, then the product a × b equals c × d and represents the total number of atoms exchanged in the reaction. The concept of the isotopic exchange reaction is best shown by an example. Consider the exchange of deuterium between water and hydrogen gas. This may be written as a reaction among isotopically homogeneous molecules; that is, . . . H2O + D2 = D2O + H2 (2.2a) . . . or, alternatively, as exchange between homogeneous and heterogeneous molecules: . . . H2O + HD = HDO + H2 (2.2b) . . . Much of the utility of isotopic exchange reactions is that they may be described by equilibrium constants, defined in the standard way as the quotient of the activities of the products and reactants. Thus, the equilibrium condition for equation 2.2b becomes . . . K = ([HDO][H2])/([H2O][HD]) (2.3) . . . where K is the equilibrium constant. In equation 2.3, K has a particularly high value of 3.7 at 25°C.


1982 ◽  
Vol 35 (2) ◽  
pp. 237 ◽  
Author(s):  
DV Fenby ◽  
GL Bertrand

Bertrand and Burchfield proposed that the equilibrium constants K and the (standard) enthalpies ΔH of isotopic exchange reactions are related by the equation K = Kstatexp(-ΔH/RT) in which Kstat is the statistical (random) equilibrium constant. The application of this equation to deuterium exchange reactions for which experimental K and ΔH values are available suggests that it is a good approximation at 298 K. In this paper we present a statistical mechanical analysis to account for the success of the equation and to point out its limitations.


1947 ◽  
Vol 15 (5) ◽  
pp. 261-267 ◽  
Author(s):  
Jacob Bigeleisen ◽  
Maria Goeppert Mayer

1973 ◽  
Vol 28 (2) ◽  
pp. 129-136 ◽  
Author(s):  
J. Bron ◽  
Chen Fee Chang ◽  
M. Wolfsberg

Ideal gas phase isotopic partition function ratios involving both deuterium and tritium substitution for hydrogen and also heavy atom substitution in H2, H2O, H2S, H2Se, and NH3 have been calculated at a number of temperatures. The results have been least squares fitted to a five term series in powers of (300/T). Various correction factors to the harmonic approximation were considered in the calculation of the partition function ratios. It is demonstrated that the tabulated ratios can be used to calculate equilibrium constants for isotopic exchange reactions.


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