The competing unimolecular dissociations of a variety of proton-bound pairs of amino compounds of formula
R1NH2, R1R2NH, where R1 and R2 are chiefly alkyl groups C1 to C9, have been investigated by tandem mass
spectrometry. Metastable and collision-induced dissociations were studied. The relative product yields, [B1H+]/[B2H+], from B1H+B2 ions (B
n
= amine) have been related to the proton affinities (PA) of B1 and B2 by the
kinetic method. In its simplest form, the method assumes no entropy effects and a zero reverse energy barrier
for the competing dissociations. The general effects expected from nonzero entropies of activation are described
in terms of how they influence log(rate constant) vs internal energy plots for such competing dissociations.
For these homologous series such effects were observed to be minimal and the kinetic method well reproduces
most of the reference PA values. In view of the very close agreement between many reference PA values
obtained from equilibrium studies, it is possible that small reverse energy barriers (ca. 5 kJ mol-1) may be
identifiable by the kinetic method, in particular for t-C4H9NH2, the homologous di-n-alkylamines, and possibly
larger barriers for di-sec-alkylamines. The method is quite sensitive to small discrepancies in PA, and new
values have been proposed for benzylamine, 924 ± 4 kJ mol-1, (CH3)(n-C4H9)NH, 951 ± 4 kJ mol-1, and
(i-C4H9)2NH, 969 ± 4 kJ mol-1. Results have also been obtained for some bidentate species, the 1,2-, 1,3-,
and 1,4-diaminoethane, propane, and butane, respectively. Particular attention was given to the effects of
activation entropies, ΔS
⧧, and the possible presence of reverse energy barriers, E
rev, both of which are here
a significant problem for the kinetic method. It was found that for 1,2-diaminoethane there was a ΔS
⧧ effect,
particularly for collisionally activated ions. The derived PA of 949 ± 4 kJ mol-1 is quite close to the reference
value for this compound, 952 ± 4 kJ mol-1. It was concluded that for 1,3-diaminopropane (reference PA 987
± 4 kJ mol-1), the method failed due both to an activation entropy effect and the presence of a reverse
energy barrier. The latter was estimated to be ca. 20 kJ mol-1, making ca. 967 kJ mol-1 the apparent PA
resulting from the kinetic method. For 1,4-diaminobutane (reference PA = 1006 ± 4 kJ mol-1), here too the
kinetic method failed and similar difficulties arose with an estimated reverse energy barrier of ca. 32 kJ
mol-1. The overall results for these three compounds were compared with a recent report in this journal on
low-energy collision-induced fragmentations. These results for species having a bidentate structure indicate
that similar difficulties may apply to biomolecules and that PA values obtained by the kinetic method may
be flawed.