Sandra Osburn

Sequence-scrambling fragmentation pathways of protonated peptides.

The gas-phase structures and fragmentation pathways of the N-terminal b and a fragments of YAGFL-NH(2), AGLFY-NH(2), GFLYA-NH(2), FLYAG-NH(2), and LYAGF-NH(2) were investigated using collision-induced dissociation (CID) and detailed molecular mechanics and density functional theory (DFT) calculations. Our combined experimental and theoretical approach allows probing of the scrambling and rearrangement reactions that take place in CID of b and a ions. It is shown that low-energy CID of the b(5) fragments of the above peptides produces nearly the same dissociation patterns. Furthermore, CID of protonated cyclo-(YAGFL) generates the same fragments with nearly identical ion abundances when similar experimental conditions are applied. This suggests that rapid cyclization of the primarily linear b(5) ions takes place and that the CID spectrum is indeed determined by the fragmentation behavior of the cyclic isomer. This can open up at various amide bonds, and its fragmentation behavior can be understood only by assuming a multitude of fragmenting linear structures. Our computational results fully support this cyclization-reopening mechanism by showing that protonated cyclo-(YAGFL) is energetically favored over the linear b(5) isomers. Furthermore, the cyclization-reopening transition structures are energetically less demanding than those of conventional bond-breaking reactions, allowing fast interconversion among the cyclic and linear isomers. This chemistry can lead in principle to complete loss of sequence information upon CID, as documented for the b(5) ion of FLYAG-NH(2). CID of the a(5) ions of the above peptides produces fragment ion distributions that can be explained by assuming b-type scrambling of their parent population and a --> a*-type rearrangement pathways ( Vachet , R. W. , Bishop , B. M. , Erickson , B. W. , and Glish , G. L. J. Am. Chem. Soc. 1997, 119, 5481 ). While a ions easily undergo cyclization, the resulting macrocycle predominantly reopens to regenerate the original linear structure. Computational data indicate that the a --> a*-type rearrangement pathways of the linear a isomers involve post-cleavage proton-bound dimer intermediates in which the fragments reassociate and the originally C-terminal fragment is transferred to the N-terminus.

Influence of size on apparent scrambling of sequence during CID of b-type ions

We investigated the influence of peptide size on the apparent loss of sequence during collision-induced dissociation (CID) of b ions using a group of peptides containing from between 4 and 10 residues. Although scrambling of sequence for b3+ generated from tetrapeptides is minimal, significant formation of nondirect sequence ions (i.e., ions for which scrambling has apparently occurred) was observed for all larger b ions included in the study.

Structure and Reactivity of the Cysteine Methyl Ester Radical Cation

The structure and reactivity of the cysteine methyl ester radical cation, CysOMe(.+) , have been examined in the gas phase using a combination of experiment and density functional theory (DFT) calculations. CysOMe(.+) undergoes rapid ion-molecule reactions with dimethyl disulfide, allyl bromide, and allyl iodide, but is unreactive towards allyl chloride. These reactions proceed by radical atom or group transfer and are consistent with CysOMe(.+) possessing structure 1, in which the radical site is located on the sulfur atom and the amino group is protonated. This contrasts with DFT calculations that predict a captodative structure 2, in which the radical site is positioned on the α carbon and the carbonyl group is protonated, and that is more stable than 1 by 13.0 kJ mol(-1) . To resolve this apparent discrepancy the gas-phase IR spectrum of CysOMe(.+) was experimentally determined and compared with the theoretically predicted IR spectra of a range of isomers. An excellent match was obtained for 1. DFT calculations highlight that although 1 is thermodynamically less stable than 2, it is kinetically stable with respect to rearrangement.

Influence of amino acid side chains on apparent selective opening of cyclic b5 ions

In this study, the possible influence of acidic, basic, and amide side chains on the opening of a putative macrocyclic b ion (b5+) intermediate was investigated. Collision induced dissociation (CID) of b5 ions was studied using a group of hexapeptides in which amino acids with the side chains of interest occupied internal sequence positions. Further experiments were performed with permuted isomers of glutamine (Q) containing peptides to probe for sequence scrambling and whether the specific sequence site of the residues influences opening of the macrocycle. Overall, the trend for (apparent) preferential/selective opening of the cyclic b5+, presumably due to the side chain, followed by the loss of the amino acid with active side group is: Q > K > D > N ∼ E.

Structure and reactivity of a(n) and a(n) peptide fragments investigated using isotope labeling, tandem mass spectrometry, and density functional theory calculations.

Extensive 15N labeling and multiple-stage tandem mass spectrometry were used to investigate the fragmentation pathways of the model peptide FGGFL during low-energy collision-induced-dissociation (CID) in an ion-trap mass spectrometer. Of particular interest was formation of a4 from b4 and a*4 (a4-NH3) from a4 ions correspondingly, and apparent rearrangement and scrambling of peptide sequence during CID. It is suggested that the original FGGFoxab4 structure undergoes b-type scrambling to form GGFFoxa. These two isomers fragment further by elimination of CO and 14NH3 or 15NH3 to form the corresponding a4and a*4 isomers, respectively. For (15N-F)GGFL and FGG(15N-F)L the a*4 ion population appears as two distinct peaks separated by 1 mass unit. These two peaks could be separated and fragmented individually in subsequent CID stages to provide a useful tool for exploration of potential mechanisms along the a4 → a*4 pathway reported previously in the literature (Vachet et al. J. Am. Chem. Soc.1997, 119, 5481, and Cooper et al. J. Am. Soc. Mass Spectrom.2006, 17, 1654). These mechanisms result in formally the same a*4 structures but differ in the position of the expelled nitrogen atom. Detailed analysis of the observed fragmentation patterns for the separated light and heavy a*4 ion fractions of (15N-F)GGFL indicates that the mechanism proposed by Cooper et al. is consistent with the experimental findings, while the mechanism proposed by Vachet et al. cannot account for the labeling data. In addition, a new rearrangement pathway is presented for a4*-CO ions that effectively transfers the former C-terminal amino acid residue to the N-terminus.

Structure and Reactivity of Homocysteine Radical Cation in the Gas Phase Studied by Ion–Molecule Reactions and Infrared Multiple Photon Dissociation

The reactivity of the cysteine (Cys) and homocysteine (Hcy) radical cation was studied using ion-molecule reactions. The radical cations were generated via collision-induced dissociation (CID) of their S-nitrosylated precursors. Cleavage of the S-NO bond led to the formation of the radical initially positioned on the sulfur atom. The reactions of the radical cations with dimethyl disulfide revealed that the cysteine radical cation reacts more quickly than the homocysteine radical cation. Infrared multiple photon dissociation (IRMPD) spectroscopy and density functional theory (DFT) calculations were used to determine the structure of the homocysteine radical cation, which was compared to the previously published structure of the cysteine radical cation (Sinha et al. Phys. Chem. Chem. Phys. 2010, 12, 9794-9800). IRMPD spectroscopy and DFT calculations revealed that this difference in radical reactivity was not a result of a radical rearrangement for the homocysteine radical cation but rather that the reactivity was modulated by stronger hydrogen bonding.

Cobalt-Mediated Decarboxylative Homocoupling of Alkynyl Carboxylic Acids

Cobalt-mediated decarboxylative Glaser-like C–C bond coupling of carboxylates has been studied in the gas phase using collision-induced dissociation (CID) multistage mass spectrometry (MSn) experiments. Both the identity of the carboxylate RCO2– (R = Me, HC≡C, MeC≡C, and PhC≡C) and the nuclearity of the complex ([CoCl(O2CR)2]– versus [Co2Cl3(O2CR)2]–) play a role in the types of reactions observed and their relative activation energies. In the first stage of CID, the mononuclear complex [CoCl(O2CMe)2]– undergoes decarboxylation, while the dinuclear [Co2Cl3(O2CMe)2]– undergoes cluster fission to yield [CoCl3]–; all acetylenic carboxylate complexes [CoCl(O2CR)2]– and [Co2Cl3(O2CR)2]– undergo decarboxylation. Isolation of the decarboxylated products followed by a second stage of CID results in a second decarboxylation event for all systems except for [CoCl(Me)(O2CMe)]–, which undergoes bond homolysis. In the final stage of CID, all acetylenic complexes undergo Glaser coupling, forming reduced Co anions. Overall dinuclear cobalt clusters are superior to mononuclear complexes at promoting decarboxylation and reductive coupling. The order of reactivity among the acetylide ligands is PhC≡C > MeC≡C > HC≡C.

Post-translational modification in the gas phase: mechanism of cysteine S-nitrosylation via ion-molecule reactions.

The gas-phase mechanism of S-nitrosylation of thiols was studied in a quadrupole ion trap mass spectrometer. This was done via ion-molecule reactions of protonated cysteine and many of its derivatives and other thiol ions with neutral tert-butyl nitrite or nitrous acid. Our results showed that the presence of the carboxylic acid functional group, -COOH, in the vicinity of the thiol group is essential for the gas-phase nitrosylation of thiols. When the carboxyl proton is replaced by a methyl group (cysteine methyl ester) no nitrosylation was observed. Other thiols lacking a carboxylic acid functional group displayed no S-nitrosylation, strongly suggesting that the carboxyl hydrogen plays a key role in the nitrosylation process. These results are in excellent agreement with a solution-phase mechanism proposed by Stamler et al. (J. S. Stamler, E. J. Toone, S. A. Lipton, N. J. Sucher. Neuron 1997, 18, 691-696) who suggested a catalytic role for the carboxylic acid group adjacent to cysteine residues and with later additions by Ascenzi et al. (P. Ascenzi, M. Colasanti, T. Persichini, M. Muolo, F. Polticelli, G. Venturini, D. Bordo, M. Bolognesi. Biol. Chem. 2000, 381, 623-627) who postulated that the presence of the carboxyl in the cysteine microenvironment in proteins is crucial for S-nitrosylation. A concerted mechanism for the gas-phase S-nitrosylation was proposed based on our results and was further studied using theoretical calculations. Our calculations showed that this proposed pathway is exothermic by 44.0 kJ mol(-1). This is one of the few recent examples when a gas-phase mechanism matches one in solution.

Role of Hydrogen Bonding on the Reactivity of Thiyl Radicals: A Mass Spectrometric and Computational Study Using the Distonic Radical Ion Approach

Experimental and computational quantum chemistry investigations of the gas-phase ion-molecule reactions between the distonic ions +H3N(CH2)nS• (n = 2-4) and the reagents dimethyl disulfide, allyl bromide, and allyl iodide demonstrate that intramolecular hydrogen bonding can modulate the reactivity of thiyl radicals. Thus, the 3-ammonium-1-propanethiyl radical (n = 3) exhibits the lowest reactivity of these distonic ions toward all substrates. Theoretical calculations on this distonic ion highlight that its most stable conformation involves a six-membered ring configuration, and that it has the strongest intramolecular hydrogen bond. In addition, the calculations indicate that the barrier heights for radical abstraction by this hydrogen-bond-stabilized 3-ammonium-1-propanethiyl radical are the highest among the systems examined, consistent with the experimental observations.

Gas-phase tyrosine-to-cysteine radical migration in model systems

Radical migration, both intramolecular and intermolecular, from the tyrosine phenoxyl radical Tyr(O•) to the cysteine radical Cys(S•) in model peptide systems was observed in the gas phase. Ion–molecule reactions (IMRs) between the radical cation of homotyrosine and propyl thiol resulted in a fast hydrogen atom transfer. In addition, radical cations of the peptide LysTyrCys were formed via two different methods, affording regiospecific production of Tyr(O•) or Cys(S•) radicals. Collision-induced dissociation of these isomeric species displayed evidence of radical migration from the oxygen to sulfur, but not for the reverse process. This was supported by theoretical calculations, which showed the Cys(S•) radical slightly lower in energy than the Tyr(O•) isomer. IMRs of the LysTyrCys radical cation with allyl iodide further confirmed these findings. A mechanism for radical migration involving a proton shuttle by the C-terminal carboxylic group is proposed.