Paul D. Schnier

Tandem mass spectrometry of large biomolecule ions by blackbody infrared radiative dissociation

A new method for the dissociation of large ions formed by electrospray ionization is demonstrated. Ions trapped in a Fourier transform mass spectrometer at pressures below 10(-)(8) Torr are dissociated by elevating the vacuum chamber to temperatures up to 215 °C. Rate constants for dissociation are measured and found to be independent of pressure below 10(-)(7) Torr. This indicates that the ions are activated by absorption of blackbody radiation emitted from the chamber walls. Dissociation efficiencies as high as 100% are obtained. There is no apparent mass limit to this method; ions as large as ubiquitin (8.6 kDa) are readily dissociated. Thermally stable ions, such as melittin 3+ (2.8 kDa), did not dissociate at temperatures up to 200 °C. This method is highly selective for low-energy fragmentation, from which limited sequence information can be obtained. From the temperature dependence of the dissociation rate constants, Arrhenius activation energies in the low-pressure limit are obtained. The lowest energy dissociation processes for the singly and doubly protonated ions of bradykinin are loss of NH(3) and formation of the b(2)/y(7) complementary pair, with activation energies of 1.3 and 0.8 eV, respectively. No loss of NH(3) is observed for the doubly protonated ion; some loss of H(2)O occurs. These results show that charge-charge interactions not only lower the activation energy for dissociation but also can dramatically change the fragmentation, most likely through changes in the gas-phase conformation of the ion. Dissociation of ubiquitin ions produces fragmentation similar to that obtained by IRMPD and SORI-CAD. Higher charge state ions dissociate to produce y and b ions; the primary fragmentation process for low charge state ions is loss of H(2)O.

On the maximum charge state and proton transfer reactivity of peptide and protein ions formed by electrospray ionization

A relatively simple model for calculation of the energetics of gas-phase proton transfer reactions and the maximum charge state of multiply protonated ions formed by electrospray ionization is presented. This model is based on estimates of the intrinsic proton transfer reactivity of sites of protonation and point charge Coulomb interactions. From this model, apparent gas-phase basicities (GBapp) of multiply protonated ions are calculated. Comparison of this value to the gas-phase basicity of the solvent from which an ion is formed enables a maximum charge state to be calculated. For 13 commonly electrosprayed proteins, our calculated maximum charge states are within an average of 6% of the experimental values reported in the literature. This indicates that the maximum charge state for proteins is determined by their gas-phase reactivity. Similar results are observed for peptides with many basic residues. For peptides with few basic residues, we find that the maximum charge state is better correlated to the charge state in solution. For low charge state ions, we find that the most basic sites Arg, Lys, and His are preferentially protonated. A significant fraction of the less basic residues Pro, Trp, and Gln are protonated in high charge state ions. The calculated GBapp of individual protonation sites varies dramatically in the high charge state ions. From these values, we calculate a reduced cross section for proton transfer reactivity that is significantly lower than the Langevin collision frequency when the GBapp of the ion is approximately equal to the GB of the neutral base.

Hepcidin revisited, disulfide connectivity, dynamics, and structure.

Hepcidin is a tightly folded 25-residue peptide hormone containing four disulfide bonds, which has been shown to act as the principal regulator of iron homeostasis in vertebrates. We used multiple techniques to demonstrate a disulfide bonding pattern for hepcidin different from that previously published. All techniques confirmed the following disulfide bond connectivity: Cys1–Cys8, Cys3–Cys6, Cys2–Cys4, and Cys5–Cys7. NMR studies reveal a new model for hepcidin that, at ambient temperatures, interconverts between two different conformations, which could be individually resolved by temperature variation. Using these methods, the solution structure of hepcidin was determined at 325 and 253 K in supercooled water. X-ray analysis of a co-crystal with Fab appeared to stabilize a hepcidin conformation similar to the high temperature NMR structure.

Reliable determinations of protein-ligand interactions by direct ESI-MS measurements: Are we there yet?

The association-dissociation of noncovalent interactions between protein and ligands, such as other proteins, carbohydrates, lipids, DNA, or small molecules, are critical events in many biological processes. The discovery and characterization of these interactions is essential to a complete understanding of biochemical reactions and pathways and to the design of novel therapeutic agents that may be used to treat a variety of diseases and infections. Over the last 20 y, electrospray ionization mass spectrometry (ESI-MS) has emerged as a versatile tool for the identification and quantification of protein–ligand interactions in vitro. Here, we describe the implementation of the direct ESI-MS assay for the determination of protein–ligand binding stoichiometry and affinity. Additionally, we outline common sources of error encountered with these measurements and various strategies to overcome them. Finally, we comment on some of the outstanding challenges associated with the implementation of the assay and highlight new areas where direct ESI-MS measurements are expected to make significant contributions in the future.

Resolving disulfide structural isoforms of IgG2 monoclonal antibodies by ion mobility mass spectrometry.

Recombinant monoclonal antibodies are an important class of therapeutic agents that have found widespread use for the treatment of many human diseases. Here, we have examined the utility of ion mobility mass spectrometry (IMMS) for the rapid characterization of disulfide variants in intact IgG2 monoclonal antibodies. It is shown that IMMS reveals 2 to 3 gas-phase conformer populations for IgG2s. In contrast, a single gas-phase conformer is revealed using IMMS for both an IgG1 antibody and a Cys-232 --> Ser mutant IgG2, both of which are homogeneous with respect to disulfide bonding. This provides strong evidence that the observed IgG2 gas-phase conformers are related to disulfide bond heterogeneity. Additionally, IMMS analysis of redox enriched disulfide isoforms allows assignment of the mobility peaks to established disulfide bonding patterns. These data clearly illustrate how IMMS can be used to quickly provide information on the higher order structure of antibody therapeutics.

Hydrophobic protein-ligand interactions preserved in the gas phase.

The results of time-resolved thermal dissociation measurements and molecular dynamic simulations are reported for gaseous deprotonated ions of the specific complexes of bovine beta-lactoglobulin (Lg) and a series of the fatty acids (FA): CH(3)(CH(2))(x)COOH, where x = 10, 12, 14, and 16. At the reaction temperatures investigated, 25-66 degrees C, the gaseous ions dissociate exclusively by the loss of neutral FA. According to the kinetic data, and confirmed by ion mobility measurements, the (Lg + FA)(7-) ions exist in two, noninterconverting structures designated the fast (Lg + FA)(f)(7-) and slow (Lg + FA)(s)(7-) components. The Arrhenius parameters for both components are sensitive to the length of the FA aliphatic chain. For the fast components, the activation energy (E(a)) increases in a nearly linear fashion, with each methylene group contributing approximately 0.8 kcal mol(-1) to E(a). This is similar to the contribution of -CH(2)- groups to the solvation of n-alkanes in nonpolar solvents. Furthermore, the magnitude of the E(a) values for the fast components is similar to the solvation enthalpies expected for the FA aliphatic chains in nonpolar and weakly polar solvents. The E(a) values determined for the slow components are larger than those of the fast components. Furthermore, the E(a) values do not vary in a simple fashion with the length of the aliphatic chain. Molecular dynamics simulations performed on the (Lg + PA) complex revealed that, depending on the charge configuration, the (Lg + PA)(7-) ion can exist in two distinct structures, which differ primarily by the position of the EF loop. In the open structure the EF loop is positioned away from the entrance to the hydrophobic cavity and the ligand is stabilized only through nonpolar intermolecular interactions. In the closed structure the EF loop covers the entrance of the cavity and the carboxylic group of PA participates in H-bonds with residues on the EF loop or residues located at the entrance of the cavity. The loss of ligand from the closed structure would require both the cleavage of the H-bonds and the nonpolar contacts. Taken together, these results suggest that the aliphatic chain of the FA remains bound within the hydrophobic cavity in the gas phase (Lg + FA)(7-) ions. Furthermore, the barrier to dissociation of the (Lg + FA)(f)(7-) ions reflects predominantly the cleavage of the nonpolar intermolecular interactions, while for the (Lg + FA)(s)(7-) ions the FA is stabilized by both nonpolar interactions and H-bonds.

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

The dissociation kinetics of protonated leucine enkephalin and its proton and alkali metal bound dimers were investigated by blackbody infrared radiative dissociation in a Fouriertransform mass spectrometer. From the temperature dependence of the unimolecular dissociation rate constants, Arrhenius activation parameters in the zero-pressure limit are obtained. Protonated leucine enkephalin dissociates to form b4 and (M-H2O)+ ions with an average activation energy (Ea) of 1. 1 eV and an A factor of 1010. 5 s−1. The value of the A factor indicates that these dissociation processes are rearrangements. The b4 ions subsequently dissociate to form a4 ions via a process with a relatively high activation energy (1.3 eV), but one that is entropically favored. For the cationized dimers, the thermal stability decreases with increasing cation size, consistent with a simple electrostatic interaction in these noncovalent ion-molecule complexes. The Ea and A factors are indistinguishable within experimental error with values of ∼1.5 eV and 1017 s−1, respectively. Although not conclusive, results from master equation modeling indicate that all these BIRD processes, except for b4 → a4, are in the rapid energy exchange limit. In this limit, the internal energy of the precursor ion population is given by a Boltzmann distribution and information about the energetics and dynamics of the reaction are obtained directly from the measured Arrhenius parameters.

Gas Phase Stabilization of Noncovalent Protein Complexes Formed by Electrospray Ionization

The use of gas phase additives to stabilize noncovalent protein complexes in electrospray ionization mass spectrometry (ES-MS) is demonstrated for two protein-ligand interactions, an enzyme-small molecule inhibitor complex, and a protein-disaccharide complex. It is shown that the introduction of gas phase imidazole into the ES ion source effectively protects gas phase protein-ligand complexes against in-source dissociation. The stabilizing effect of imidazole vapor is comparable to that observed upon addition of imidazole to the ES solution. The introduction of sulfur hexafluoride, at high partial pressure, into the source region also effectively suppresses in-source dissociation of protein complexes. It is proposed that evaporative cooling is the primary mechanism responsible for the stabilizing effects observed for the gas phase additives.

Ordering of the N-terminus of human MDM2 by small molecule inhibitors.

Restoration of p53 function through the disruption of the MDM2-p53 protein complex is a promising strategy for the treatment of various types of cancer. Here, we present kinetic, thermodynamic, and structural rationale for the remarkable potency of a new class of MDM2 inhibitors, the piperidinones. While these compounds bind to the same site as previously reported for small molecule inhibitors, such as the Nutlins, data presented here demonstrate that the piperidinones also engage the N-terminal region (residues 10-16) of human MDM2, in particular, Val14 and Thr16. This portion of MDM2 is unstructured in both the apo form of the protein and in MDM2 complexes with p53 or Nutlin, but adopts a novel β-strand structure when complexed with the piperidinones. The ordering of the N-terminus upon binding of the piperidinones extends the current model of MDM2-p53 interaction and provides a new route to rational design of superior inhibitors.

Blackbody infrared radiative dissociation of oligonucleotide anions

The dissociation kinetics of a series of doubly deprotonated oligonucleotide 7-mers [d(A)72−, d(AATTAAT)2−, d(TTAATTA)2−, and d(CCGGCCG)2−] were measured using blackbody infrared radiative dissociation in a Fourier-transform mass spectrometer. The oligonucleotides dissociate first by cleavage at the glycosidic bond leading to the loss of a neutral nucleobase, followed by cleavage at the adjacent (5′) phosphodiester bond to produce structurally informative a-base and w type ions. From the temperature dependence of the unimolecular dissociation rate constants, Arrhenius activation parameters in the zero-pressure limit are obtained for the loss of base. The measured Arrhenius parameters are dependent on the identity of the nucleobase. The process involving the loss of an adenine base from the dianions, d(A)72−, d(AATTAAT)2−, and d(TTAATTA)2− has an average activation energy (Ea) of ∼1.0 eV and a preexponential factor (A) of 1010 s−1. Both guanine and cytosine base loss occurs for d(CCGGCCG)2−. The average Arrhenius parameters for the loss of cytosine and guanine are Ea=1.32 ± 0.03 eV and A=1013.3±0.3 s−1. No loss of thymine was observed for mixed adenine-thymine oligonucleotides. Neither base loss nor any other fragmentation reactions occur for d(T)72− over a 600 s reaction delay at 207 °C, a temperature close to the upper limit accessible with our instrument. The Arrhenius parameters indicate that the preferred cleavage sites for mixed oligonucleotides of similar mass-to-charge ratio will be strongly dependent on the internal energy of the precursor ions. At low internal energies (effective temperatures below 475 K), loss of adenine and subsequent cleavage of the adjacent phosphoester bonds will dominate, whereas at higher energies, preferential cleavage at C and G residues will occur. The magnitude of the A factors ≤1013 s−1 measured for the loss of the three nucleobases (A, G, and C) is indicative of an entropically neutral or disfavored process as the rate limiting step for this reaction.