DISSOCIATION ENERGETICS AND MECHANISMS OF LEUCINE-ENKEPHALIN (M+H)(+)AND (2M+X)(+) IONS (X=H, LI, NA, K, AND RB) MEASURED BY BLACKBODY INFRARED RADIATIVE DISSOCIATION

Citation
Pd. Schnier et al., DISSOCIATION ENERGETICS AND MECHANISMS OF LEUCINE-ENKEPHALIN (M+H)(+)AND (2M+X)(+) IONS (X=H, LI, NA, K, AND RB) MEASURED BY BLACKBODY INFRARED RADIATIVE DISSOCIATION, Journal of the American Society for Mass Spectrometry, 8(8), 1997, pp. 771-780
Citations number
40
Categorie Soggetti
Chemistry Physical","Chemistry Analytical",Spectroscopy
ISSN journal
10440305
Volume
8
Issue
8
Year of publication
1997
Pages
771 - 780
Database
ISI
SICI code
1044-0305(1997)8:8<771:DEAMOL>2.0.ZU;2-B
Abstract
The dissociation kinetics of protonated leucine enkephalin and its pro ton and alkali metal bound dimers were investigated by blackbody infra red radiative dissociation in a Fourier-transform mass spectrometer. F rom the temperature dependence of the unimolecular dissociation rate c onstants, Arrhenius activation parameters in the zero-pressure limit a re obtained. Protonated leucine enkephalin dissociates to form b(4) an d (M-H2O)(+) ions with an average activation energy (E-a) of 1.1 eV an d an A factor of 10(10.5) s(-1). The value of the A factor indicates s that these dissociation processes are rearrangements. The b(4) ions s ubsequently dissociate to form a(4) ions via a process with a relative ly high activation energy (1.3 eV), but one that is entropically favor ed. For the cationized dimers, the thermal stability decreases with in creasing cation size, consistent with a simple electrostatic interacti on in these noncovalent ion-molecule complexes. The E-a and A factors are indistinguishable within experimental error with values of similar to 1.5 eV and 10(17) s(-1), respectively. Although not conclusive, re sults from master equation modeling indicate that all these BIRD proce sses, except for b(4) --> a(4), are in the rapid energy exchange limit . In this limit, the internal energy of the precursor ion population i s given by a Boltzmann distribution and information about the energeti cs and dynamics of the reaction are obtained directly from the measure d Arrhenius parameters. (C) 1997 American Society for Mass Spectrometr y.