Collision cross section (Ω) values of gas-phase ions of proteins and protein complexes are used to probe the structures of the corresponding species in solution. Ions of many proteins exhibit increasing Ω-values with increasing charge state but most Ω-values calculated for protein ions have used simple collision models that do not explicitly account for charge. Here we use a combination of ion mobility mass spectrometry experiments with helium gas and trajectory method calculations to characterize the extents to which increases in experimental Ω-values with increasing charge state may be attributed to increased momentum transfer concomitant with enhanced long-range interactions between the protein ion and helium atoms. Ubiquitin and C-to-N terminally linked diubiquitin ions generated from different solution conditions exhibit more than a 2-fold increase in Ω with increasing charge state. For native and energy-relaxed models of the proteins and most methods for distributing charge, Ω-values calculated using the trajectory method increase by less than 1% over the range of charge states observed from typical solution conditions used for native mass spectrometry. However, the calculated Ω-values increase by 10% to 15% over the full range of charge states observed from all solution conditions. Therefore, contributions from enhanced ion-induced dipole interactions with increasing charge state are significant but without additional structural changes can account for only a fraction of the increase in Ω observed experimentally. On the basis of these results, we suggest guidelines for calculating Ω-values in the context of applications in biophysics and structural biology.

Ion mobility (IM) is a gas-phase separation technique that is used to determine the collision cross sections of native-like ions of proteins and protein complexes, which are in turn used as restraints for modeling the structures of those analytes in solution. Here, we evaluate the stability of native-like ions using tandem IM experiments implemented using structures for lossless ion manipulations (SLIM). In this implementation of tandem IM, ions undergo a first dimension of IM up to a switch that is used to selectively transmit ions of a desired mobility. Selected ions are accumulated in a trap and then released after a delay to initiate the second dimension of IM. For delays ranging from 16 to 33 231 ms, the collision cross sections of native-like, 7+ cytochrome c ions increase monotonically from 15.1 to 17.1 nm2. The largest products formed in these experiments at near-ambient temperature are still far smaller than those formed in energy-dependent experiments (∼21 nm2). However, the collision cross section increases by ∼2% between delay times of 16 and 211 ms, which may have implications for other IM experiments on these time scales. Finally, two subpopulations from the full population were each mobility selected and analyzed as a function of delay time, showing that the three populations can be differentiated for at least 1 s. Together, these results suggest that elements of native-like structure can have long lifetimes at near-ambient temperature in the gas phase but that gas-phase dynamics should be considered when interpreting results from IM.

The fidelity between the structures of proteins in solution and protein ions in the gas phase is critical to experiments that use gas-phase measurements to infer structures in solution. Here we generate ions of lysozyme, a 129-residue protein whose native tertiary structure contains four internal disulfide bonds, from three solutions that preserve varying extents of the original native structure. We then use cation-to-anion proton-transfer reactions (CAPTR) to reduce the charge states of those ions in the gas phase and ion mobility to probe their structures. The collision cross section (Ω) distributions of each CAPTR product depends to varying extents on the original solution, the charge state of the product, and the charge state of the precursor. For example, the Ω distributions of the 6+ ions depend strongly on the original solutions conditions and to a lesser extent on the charge state of the precursor. Energy-dependent experiments suggest that very different structures are accessible to disulfide-reduced and disulfide-intact ions, but similar Ω distributions are formed at high energy for disulfide-intact ions from denaturing and from aqueous conditions. The Ω distributions of the 3+ ions are all similar but exhibit subtle differences that depend more strongly on the original solutions conditions than other factors. More generally, these results suggest that specific CAPTR products may be especially sensitive to specific elements of structure in solution.

Ion mobility (IM) separates ions based on their response to an electric field in the presence of a drift gas. Because of its speed and sensitivity, the integration of IM and mass spectrometry (MS) offers many potential advantages for the analysis of small molecules. To determine the effects that drift gas selection has on the information content of IM separations, absolute collision cross sections (Ω) with He, N2, Ar, CO2, and N2O were measured for the 20 common amino acids using low-pressure, ambient-temperature ion mobility experiments performed in a radio frequency-confining drift cell. The drift gases were selected to span a range of masses, geometries, and polarizabilities. The information content of each separation was quantified using its peak capacity, which depended on factors contributing to widths of peaks as well as the range of Ω relative to the average Ω for the analytes. The selectivity of each separation was quantified by calculating the peak-to-peak resolution for each pairwise combination of amino acid ions. The number of pairs that were resolved depended strongly on the peak capacity, but the identities of the pairs resolved also depended on the drift gas. Therefore, results using different drift gases are partially orthogonal and provide complementary chemical information. The temperatures and pressures used for these experiments are similar to those used in many IM-MS instruments, therefore, the outcomes of this research are applicable to optimizing the information content of a wide range of contemporary and future IM-MS experiments.

•Droplet size distributions are measured over a range of ionization currents.•Droplet sizes increase with increasing ionization current.•Nonspecific aggregation characterized using Poisson statistics and experiments.•Typical native MS conditions preserve solution-phase oligomer distributions.Native mass spectrometry is widely used to determine the stoichiometries and binding constants of noncovalent interactions in solution. One challenge is that multiple analytes in a single electrospray droplet can aggregate during solvent evaporation, which will bias the distribution of oligomeric states observed during gas-phase measurements. Here, measurements of solution flow rates, electrospray currents, droplet size distributions, and nonspecific aggregation are used in conjunction with Poisson statistics to characterize the factors that control nonspecific aggregation during typical native mass spectrometry experiments. Using electrokinetic nanoelectrospray ionization and a 30 nA current, low flow rates of less than 10 nL min−1 and initial droplets with mean diameters of ∼60 nm were observed. For solutions containing 4 μM analyte under these conditions, Poisson statistics and charge-reduction drift tube ion mobility spectrometry both indicate that ∼90% of the desolvated, occupied droplets contain a single analyte. Initial droplet sizes and contributions from nonspecific aggregates both increase with increasing current. Ion mobility mass spectrometry analysis of the ions produced using these conditions without charge reduction exhibit even less nonspecific aggregation (∼2%). All approaches indicate that increasing the ionization current increases the flow rate, droplet size distribution, and extent of nonspecific aggregation. These results provide detailed insights into the role of small initial droplets in the success of native mass spectrometry.Download high-res image (231KB)Download full-size image

The structure and folding of a protein in solution depends on noncovalent interactions within the protein and those with surrounding ions and molecules. Decoupling these interactions in solution is challenging, which has hindered the development of accurate physics-based models for structure prediction. Investigations of proteins in the gas phase can be used to selectively decouple factors affecting the structures of proteins. Here, we use cation-to-anion proton-transfer reactions (CAPTR) to reduce the charge states of denatured ubiquitin ions in the gas phase, and ion mobility to probe their structures. In CAPTR, a precursor charge state is selected (P) and reacted with monoanions to generate charge-reduced product ions (C). Following each CAPTR event, denatured ubiquitin ions (13+ to 6+) yield products that rapidly isomerize to structures that have smaller collision cross sections (Ω). The Ω values of CAPTR product ions depend strongly on C and very weakly on P. Pre- and post-CAPTR activation was then used to probe the potential-energy surfaces of the precursor and product ions, respectively. Post-CAPTR activation showed that ions of different P fold differently and populate different regions of the potential-energy surface of that ion. Finally, pre-CAPTR activation showed that the structures of protein ions can be indirectly investigated using ion mobility of their CAPTR product ions, even for subtle structural differences that are not apparent from ion mobility characterization of the activated precursor ions. More generally, these results show that CAPTR strongly complements existing techniques for characterizing the structures and dynamics of biological molecules in the gas phase.

Ion mobility separation of native-like protein and protein complex ions expands the structural information available through native mass spectrometry analysis. Here, we implement Structures for Lossless Ion Manipulations (SLIM) for the analysis of native-like ions. SLIM has been shown previously to operate with near lossless transmission of ions up to 3000 Da in mass. Here for the first time, SLIM was used to separate native-like protein and protein complex ions ranging in mass from 12 to 145 kDa. The resulting arrival-time distributions were monomodal and were used to determine collision cross section values that are within 3% of those determined from radio-frequency-confining drift cell measurements. These results are consistent with the retention of native-like ion structures throughout these experiments. The apparent resolving powers of native-like ions measured using SLIM are as high as 42, which is the highest value reported directly from experimental data for the native-like ion of a protein complex. Interestingly, the apparent resolving power depends strongly on the identity of the analyte, suggesting that the arrival-time distributions of these ions may have contributions from an ensemble of structures in the gas phase that is unique to each analyte. These results suggest that the broad range of emerging SLIM technologies may all be adaptable to the analysis of native-like ions, which will enable future applications in the areas of structural biology, biophysics, and biopharmaceutical characterization.

Ion mobility mass spectrometry experiments enable the characterization of mass, assembly, and shape of biological molecules and assemblies. Here, a new radio-frequency confining drift cell is characterized and used to measure the mobilities of peptide, protein, and protein complex ions. The new drift cell replaced the traveling-wave ion mobility cell in a Waters Synapt G2 HDMS. Methods for operating the drift cell and determining collision cross section values using this experimental set up are presented within the context of the original instrument control software. Collision cross sections for 349 cations and anions are reported, 155 of which are for ions that have not been characterized previously using ion mobility. The values for the remaining ions are similar to those determined using a previous radio-frequency confining drift cell and drift tubes without radial confinement. Using this device under 2 Torr of helium gas and an optimized drift voltage, denatured and native-like ions exhibited average apparent resolving powers of 14.2 and 16.5, respectively. For ions with high mobility, which are also low in mass, the apparent resolving power is limited by contributions from ion gating. In contrast, the arrival-time distributions of low-mobility, native-like ions are not well explained using only contributions from ion gating and diffusion. For those species, the widths of arrival-time distributions are most consistent with the presence of multiple structures in the gas phase.

Ion mobility is a powerful tool for separating and characterizing the structures of ions. Here, a radio-frequency (rf) confining drift cell is used to evaluate the drift times of ions over a broad range of drift field strengths (E/P, V cm–1 Torr–1). The presence of rf potentials radially confines ions and results in excellent ion transmission at low E/P (less than 1 V cm–1 Torr–1), thereby reducing the dependence of ion transmission on the applied drift voltage. Non-linear responses between drift time and reciprocal drift voltages are observed for extremely low E/P and high rf amplitudes. Under these conditions, pseudopotential wells generated by the rf potentials dampen the mobility of ions. The effective potential approximation is used to characterize this mobility dampening behavior, which can be mitigated by adjusting rf amplitudes and electrode dimensions. Using SIMION trajectories and statistical arguments, the effective temperatures of ions in an rf-confining drift cell are evaluated. Results for the doubly charged peptide GRGDS suggest that applied rf potentials can result in a subtle increase (2 K) in effective temperature compared to an electrostatic drift tube. Additionally, simulations of native-like ions of the protein complex avidin suggest that rf potentials have a negligible effect on the effective temperature of these ions. In general, the results of this study suggest that applied rf potentials enable the measurement of drift times at extremely low E/P and that these potentials have negligible effects on ion effective temperature.