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In other work, we have shown that 10 mTorr collision gas in the first octopole is sufficient to completely thermalize the kinetic energy distribution of the electrosprayed ions, as evidenced by the disappearance of any dependence of collision-induced dissociation thresholds on the capillary temperature.
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D = 6-8 for proton transfer through a linear transition state. The argument used in the present study - attenuation of substituent and isotope effects when the rate-limiting transition state is pulled well below the entering asymptote - is, in fact, supported by the proton-transfer study.
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The observed secondary deuterium isotope effect for the acyclic metathesis reaction 2 → 3 is not attenuated at all relative to expectations from theory or solution-phase studies, while that for the ROM reaction 2 → 4 has been completely washed out. The qualitative surfaces in Schemes 4 and 5 correspond to potential energy surfaces. Inclusion of entropy - or, equivalently, transformation to free energy surfaces - would raise the transition states more than the entering asymptote because of the loss of translational and rotational entropy in the formation of a complex from two components. A quantitative treatment with RRKM theory is not possible because the real complexes are too large for a reasonable level of quantum chemical theory to calculate reliable frequencies. Nevertheless, the important comparison - the reaction of 2 → 3 versus 2 → 4 - can be made without recourse to quantitative rates.
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The strain release upon cleavage of one ring of norbornene in a ROM reaction can be estimated from exothermicity of the homodesmotic equation: (2 × ethane) + norbornene → cis-1,3-dimethylcyclopentane + Z-2-butene.
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It has been argued that while there is a difference in the π-complexation of norbornene versus cyclopentene with an unsaturated tungsten carbene, the difference is not large. Ivin, K. J.; Lapienis, G.; Rooney, J. J. Makromol. Chem. 1982, 183, 9. Also, the heats of hydrogenation of ethylene and norbornene are surprisingly similar.
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Ivin, K.J.1
Lapienis, G.2
Rooney, J.J.3
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A two-step endothermic reaction (the reverse reaction) would show an overall kinetic isotope effect that is the product of a normal equilibrium isotope effect on the reversible first step and an inverse kinetic isotope effect on the rate-determining second step. The two would largely cancel.
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Stein, S. E.; Walker, J. A.; Suryan, M. M.; Fahr, A. 23rd Symposium (International) on Combustion; The Combustion Institute: Pittsburgh, PA, 1990; pp 85-90.
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Walker, J.A.2
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Fahr, A.4
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