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Thermal decomposition kinetics of protonated peptides and peptide dimers, and comparison with surface-induced dissociation.

作者信息

Meot-Ner M, Dongré A R, Somogyi A, Wysocki V H

机构信息

Department of Chemistry, Virginia Commonwealth University, Richmond 23284-2006, USA.

出版信息

Rapid Commun Mass Spectrom. 1995;9(9):829-36. doi: 10.1002/rcm.1290090922.

DOI:10.1002/rcm.1290090922
PMID:7655076
Abstract

Rate constants for the unimolecular decomposition of peptide monomer and dimer ions by thermal and surface-induced dissociation (SID) are measured and compared. Rate constants for thermal dissociation are measured in a heated wide-bore capillary flow reactor attached in front of the capillary leading into the mass spectrometer. Thermal decomposition of the leucine enkephalin ion (YGGFL)H+ is observed between 600 and 680 K with rate constants of 20-200 s-1, and yields many of the same fragments as SID at 35 eV, although with different relative intensities. The thermal decomposition yields the Arrhenius parameters Ea = 38.3 kcal/mol, log A = 15.7. The decomposition of the monomer and dimer ions are also observed by using SID on C18 and fluorinated hydrocarbon surfaces, with rate constants of 2 x 10(4) to 40 x 10(4) s-1. The SID activated monomer ions are assigned equivalent temperatures of 710-840 K by extrapolation of the thermal activation parameters. The protonated dimer ion (YGGFL)2 H+ decomposes thermally at 500-540 K to yield the monomer ion. The dimer also decomposes by SID at low collision energies 10-20 eV on both surfaces to yield the monomer ion, and at much higher energies of 60-80 eV to yield fragments identical to the decomposition of the monomer. The large energy requirement for fragmentation from the dimer is due to energy deposition into more degrees of freedom plus the additional energy required for dissociation of the dimer to the monomer.(ABSTRACT TRUNCATED AT 250 WORDS)

摘要

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