M. Meotner et al., THERMAL-DECOMPOSITION KINETICS OF PROTONATED PEPTIDES AND PEPTIDE DIMERS, AND COMPARISON WITH SURFACE-INDUCED DISSOCIATION, Rapid communications in mass spectrometry, 9(9), 1995, pp. 829-836
Rate constants for the unimolecular decomposition of peptide monomer a
nd dimer ions by thermal and surface-induced dissociation (SID) are me
asured and compared. Rate constants for thermal dissociation are measu
red in a heated wide-bore capillary flow reactor attached in front of
the capillary leading into the mass spectrometer. Thermal decompositio
n of the leucine enkephalin ion (YGGFLH+ is observed between 600 and 6
80 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 Intensitie
s. The thermal decomposition yields the Arrhenius parameters E(a) = 38
.3 kcal/mol, log A 15.7. The decomposition of the monomer and dimer io
ns are also observed by using SID on C-18 and fluorinated hydrocarbon
surfaces, with rate constants of 2 X 10(4) to 40 X 10(4) s(-1). The SI
D activated monomer ions are assigned equivalent temperatures of 710-8
40 K by extrapolation of the thermal activation parameters. The proton
ated dimer ion (YGGFLH+ decomposes thermally at 500-540 K to yield the
monomer ion. The dimer also decomposes by SID at low collision energi
es 10-20 eV on both surfaces to yield the monomer ion, and at much hig
her energies of 60-80 eV to yield fragments identical to the decomposi
tion of the monomer. The large energy requirement for fragmentation fr
om the dimer is due to energy deposition into more degrees of freedom
plus the additional energy required for dissociation of the dimer to t
he monomer. It is assumed that the energy deposition is linear with co
llision energy up to 80 eV, and that the energy becomes randomized thr
oughout the dimer, including energy flow through the hydrogen bond(s).
These mechanistic assumptions are supported quantitatively by the SID
energy relations between monomer and dimer fragmentation. Thermal dec
omposition of the larger, multiply protonated melittin ion [M + 3H](3) occurs at substantially higher temperatures, between 810-840 K, than
those required for thermal decomposition of (YGGFLH+, to yield many o
f the same sequence ions as produced by SID at 135 eV on a fluorinated
surface.