Abstract
The analysis of intact proteins via mass spectrometry can offer several benefits to proteome characterization, although the majority of top-down experiments focus on proteoforms in a relatively low mass range (<30 kDa). Recent studies have focused on improving the analysis of larger intact proteins (up to ~75 kDa), but they have also highlighted several challenges to be addressed. One major hurdle is the efficient dissociation of larger protein ions, which often to do not yield extensive fragmentation via conventional tandem MS methods. Here we describe the first application of activated ion electron transfer dissociation (AI-ETD) to proteins in the 30–70 kDa range. AI-ETD leverages infrared photo-activation concurrent to ETD reactions to improve sequence-informative product ion generation. This method generates more product ions and greater sequence coverage than conventional ETD, higher-energy collisional dissociation (HCD), and ETD combined with supplemental HCD activation (EThcD). Importantly, AI-ETD provides the most thorough protein characterization for every precursor ion charge state investigated in this study, making it suitable as a universal fragmentation method in top-down experiments. Additionally, we highlight several acquisition strategies that can benefit characterization of larger proteins with AI-ETD, including combination of spectra from multiple ETD reaction times for a given precursor ion, multiple spectral acquisitions of the same precursor ion, and combination of spectra from two different dissociation methods (e.g., AI-ETD and HCD). In all, AI-ETD shows great promise as a method for dissociating larger intact protein ions as top-down proteomics continues to advance into larger mass ranges.
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Introduction
Top-down proteomics characterizes intact proteins, aiming to provide information about splice variants, sequence truncations, and post-translational modifications that contribute to biologically significant proteoforms [1,2,3,4]. The top-down approach continues to progress with advances in mass spectrometry (MS) and related technologies, but technical challenges have largely limited these experiments to proteins with molecular weights less than ~30 kDa [5,6,7,8]. Recent studies have focused on accessing portions of the proteome that span a larger molecular weight range (up to ~75 kDa) with some success [9,10,11], emphasizing the need for further development of instrumentation for analysis of larger protein ions, including tandem MS/MS approaches that can effectively dissociate larger protein ions.
Improving fragmentation of intact protein ions has been an active research area for decades. In the first years after electrospray ionization enabled the interrogation of large multiply charged ions, collision activated dissociation (CAD) and infrared multiphoton dissociation (IRMPD) were used to dissociate protein cations ranging from ubiquitin (8.6 kDa) to bovine serum albumin (BSA, ~66 kDa) [12,13,14,15]. Dissociation of proteins upwards of 200 kDa has also been explored [16, 17]. A limitation to slow-heating dissociation methods like CAD and IRMPD, however, is that they preferentially cleave at labile bonds, which often fails to produce suitable fragmentation for sequence elucidation. Electron capture dissociation (ECD) and electron transfer dissociation (ETD) were developed as alternatives to the so-called ergodic methods (i.e., CAD and IRMPD), offering more extensive backbone cleavage through electron-driven dissociation [18,19,20,21].
Ideally suited for highly charged cations, ECD and ETD have become indispensable tools for top-down proteomics; that said, both approaches suffer from inefficient precursor-to-product ion conversion for precursors with low charge density [22,23,24,25]. This is largely due to secondary gas-phase structure of low charge density precursors, where precursor ions adapt compact structures that increase intramolecular noncovalent interactions [26,27,28,29]. In such cases, product ions often remain together, due to the noncovalent interactions, preventing generation of sequence-informative product ions. This process is called non-dissociative electron transfer dissociation (ETnoD) [30,31,32]. Several approaches have employed supplemental activation to mitigate this problem, for example, use of higher energy electrons and collisional- or photo-activation of precursor and/or product ions [32,33,34,35,36,37,38,39,40,41,42,43,44].
Supplemental activation methods have been extensively explored for ECD with larger proteins [44,45,46,47]; fewer studies, however, have explored the effect of supplemental activation for fragmentation of larger proteins with ETD. We recently described activated-ion ETD (AI-ETD), which uses infrared photo-activation concurrent with ETD to increase product ion generation, and demonstrated that it can improve ETD efficiency for both peptide and protein precursor ions [48,49,50,51,52,53,54]. With implementation on a quadrupole-Orbitrap-linear ion trap (q-OT-LIT) hybrid MS system, we have recently shown that AI-ETD can provide near-complete sequence coverage of intact proteins in the range of molecular weights that are typically identified in top-down experiments (<25 kDa) [55]. Here we investigate the potential of AI-ETD to dissociate larger protein ions, including carbonic anhydrase (~29 kDa), aldolase (~39.2 kDa), enolase (~46.7 kDa), and BSA (~66.8 kDa). Altogether we demonstrate that AI-ETD generates significantly more sequence-informative product ions and increases overall protein characterization over ETD. The method likewise outperforms higher-energy collisional dissociation (HCD) and ETD with supplemental HCD activation (EThcD). Finally, we illustrate how different acquisition strategies, e.g., utilization of multiple ETD reaction times, can benefit top-down characterization of larger intact proteins with AI-ETD and other dissociation methods.
Materials and Methods
Sample Preparation
Carbonic anhydrase from bovine erythrocytes (UniProt Accession P00921) and bovine serum album (BSA) (UniProt Accession P02769) were purchased from Protea Biosciences (Morgantown, WV, USA). Fructose-bisphosphate aldolase A, referred to in this manuscript as aldolase, from rabbit muscle (UniProt Accession P00883), and enolase 1 from baker’s yeast (UniProt Accession P00924) were purchased from Sigma Aldrich (St. Louis, MO, USA). BSA was resuspended in buffer (8 M urea, 50 mM Tris, pH 8), reduced with 5 mM dithiothreitol for 45 min at 58 °C, alkylated with 15 mM iodoacetamide for 45 min at room temperature in the dark, and desalted using a C2 SepPak (Waters, Milford, MA, USA). All samples were resuspended at ~10 pmol/μL in 50:49.8:0.2 acetonitrile/water/formic acid prior to infusions.
Mass Spectrometry
All experiments were performed on a quadrupole-Orbitrap-linear ion trap hybrid MS system (Orbitrap Fusion Lumos; Thermo Fischer Scientific, San Jose, CA, USA) that had been previously modified to perform AI-ETD [54]. Proteins were infused at 5–10 μL/min using the instrument’s syringe pump, and precursors were ionized using electrospray ionization at 4–5 kV with respect to ground. The inlet capillary was held at 275 °C and the ion funnel rf was held at 30%. All MS/MS scans were conducted at 240,000 resolution with precursor ion targets of 800,000. For ETD, EThcD, and AI-ETD experiments, the reagent anion population was set to 300,000 ions and reaction times varied for each precursor, ranging from 5 to 40 ms. Normalized collision energies for EThcD ranged from 8 to 15, laser powers for AI-ETD ranged from 18 to 36 Watts, and normalized collision energies for HCD ranged from 15 to 25. For each precursor the optimum dissociation conditions were determined prior to data collection for HCD, ETD, EThcD, and AI-ETD. The number of microscans used was 300 for carbonic anhydrase and aldolase experiments, 400 for enolase experiments, and 500 for BSA experiments.
Data Analysis
MS/MS spectra were deconvoluted with XTRACT (Thermo Fisher Scientific) using default parameters and a S/N threshold of three. Peak lists from XTRACT and protein sequences from UniProt were loaded into ProSight Lite [56] to determine the number of matched fragments generated for each precursor and dissociation method. For combination of spectra, peak lists from each spectrum were concatenated. The “EThcD” fragmentation type, which matched b/y- and c/z-type product ions, was used for ETD, EThcD, and AI-ETD spectra, whereas “HCD”, which matched b/y-type product ions, was used for HCD spectra. All matches were made within a 10 ppm tolerance. No modifications were used for aldolase or enolase sequences, whereas carbamidomethylation of cysteines (+57.021 Da) was used for BSA and N-terminal acetylation (+42.01 Da) was used for carbonic anhydrase.
Results and Discussion
AI-ETD employs infrared photo-activation, concurrent with electron transfer ion/ion reactions, to disrupt intramolecular noncovalent interactions in precursor ions and, thereby, improve ETD reaction efficiency. The approach consistently leads to an increased number of sequence-informative product ions and to greater backbone sequence coverage of precursor proteins. To test how AI-ETD can improve ETD fragmentation of large, highly charged protein ions, we dissociated several precursor ion charge states of four protein standards that span a molecular weight range of approximately 30–70 kDa.
For carbonic anhydrase, six precursor ion charge states across the charge state envelope were selected for fragmentation with HCD, ETD, EThcD, and AI-ETD (Figure 1a). Of the four dissociation methods, AI-ETD generated the greatest sequence coverage for all six precursor ions (nearly 70%), whereas none of the other dissociation methods achieved 60% coverage (Figure 1b). Interestingly, AI-ETD improved data quality (i.e., sequence coverage, product ion count, and product ion signal) over ETD for all precursor ion charge states, whereas ETD outperformed the other supplemental activation approach, EThcD, for the highest charge states (z = 30–36). EThcD performance over ETD for the low charge states (z = 21–27) reflects similar results from a previous EThcD study of a 17.5 kDa protein [43]. All three ETD-based dissociation methods substantially outperform HCD for all six precursors, matching previous comparisons [57].
Collisional-based and electron-driven dissociation methods offer complementary fragmentation information and are often combined (following separate MS/MS events) in top-down proteomic experiments for improved identification. Figure 1c illustrates how combining HCD MS/MS results with those from AI-ETD, EThcD, or ETD MS/MS improves characterization for each of the six carbonic anhydrase precursor ions. The combination of AI-ETD and HCD provides the greatest coverage for each precursor, with a boost of approximately 8%-10% coverage over AI-ETD alone (indicated by the dashed line). Note, AI-ETD alone also provides nearly as much, if not more, sequence coverage as the combination of HCD with ETD or EThcD. When combining the best result from AI-ETD (z = 30, 69% coverage) with the best result from HCD (z = 24, 40% coverage), the total sequence coverage achieved for carbonic anhydrase is 81% with 340 total matched fragments (b-, y-, c-, and z ●-type), underscoring the known benefits of complementary dissociation methods (Figure 1d). By comparison, a previous study looking at the combination of multiple MS/MS acquisitions for carbonic anhydrase characterization showed that combining five different fragmentation conditions (including ECD, plasma ECD, and collisional activation prior to ECD, and modulation of inlet capillary temperature) can provide 77% sequence coverage [33].
Figure 2 compares ETD and AI-ETD spectra for the z = 21 charge state of carbonic anhydrase, highlighting the improved precursor-to-product ion generation afforded by AI-ETD that contributes to increased sequence coverage. AI-ETD generates 217 sequence-informative product ions to ETD’s 150 product ions, resulting in an increase of 16% sequence coverage (i.e., 66% versus 50%). The improved dissociation efficiency of AI-ETD is also apparent in the percent of total ion current (TIC) that remains in precursor ion channels, where ETD has nearly triple the amount of signal of AI-ETD in these non-informative channels (largely in charge-reduced ETnoD products). This corresponds to more than double the signal in sequence-informative product ion channels in the AI-ETD spectrum compared with ETD. Beyond simply decreasing ETnoD, AI-ETD increases product ion signal-to-noise, making successful deconvolution more likely and, thus, increasing the signal that can be leveraged for sequence elucidation.
Importantly, AI-ETD also does not significantly alter the distribution of product ion types generated from ETD. Figure 3 shows the product ion type distribution for the different dissociation methods both by count and by total intensity for the z = +30 (panel a) and z = +21 (panel b) precursor ion charge states of carbonic anhydrase. In both cases, AI-ETD increases the number of c- and z ●-type ions over ETD while maintaining similarly low amounts of b- and y-type fragments. This is in contrast to EThcD, where c- and z ●-type fragment counts are slightly lower than ETD in favor of boosts in b- and y-type ions. The gains in number of fragment ions over ETD is concomitant with increased signal in product ion channels for AI-ETD, while this is not necessarily the case with EThcD. This is likely because the beam-type collisional supplemental activation of EThcD necessitates a moderately energetic transfer of ions into a collision cell that can cause some product ion signal to be lost. Conversely, the vibrational activation via infrared photons used in AI-ETD is concurrent with ETD reactions and requires no additional shuttling of product ions into a different reaction cell. The changes (or lack thereof) in product ion distribution and intensities match previous studies on smaller peptides and proteins [43, 54, 55]. Note the data in Figure 3b further expands on the observations from Figure 2, as they are from the same precursor ion. It is also interesting to note that the y-axes scales for the count of fragment ion graphs (left graphs) is the same for Figure 3a and b, showing that AI-ETD maintains elevated product ion generation even as precursor ion charge state decreases. The capability of AI-ETD to increase generation of ETD-specific c- and z ●-type in both number and intensity while minimizing other fragment ion types is especially important for dissociation of intact proteins, where available signal can be diluted amongst the many potential product ion pathways possible from the hundreds of inter-residue bonds of the molecules [58].
Recent success of ultraviolet photodissociation (UVPD) for characterization of intact proteins makes for a natural comparison with AI-ETD. UVPD generates extensive fragmentation of peptide and protein cations, including six main fragment ion types (a-, b-, c-, x-, y-, and z-type) in addition to Y-, w-, v-, and d-ions. Although we do not have the ability to generate UVPD data in-house, three recent studies have investigated the performance of UVPD for carbonic anhydrase [57, 59, 60]. Impressively, the first description of UVPD for intact protein analysis provided 87% sequence coverage of carbonic anhydrase, the greatest sequence coverage to be reported for a protein of that size from a single acquisition [57]. More recent studies, however, have shown that UVPD can consistently provide 60%–70% sequence coverage [59, 60], making it comparable with the coverage AI-ETD can generate. Supplemental Figure 1 shows sequence coverage and product ion distributions from UVPD of carbonic anhydrase precursor ions compared with AI-ETD for the z = +30 charge state. Although no direct comparison can be made between AI-ETD and UVPD here, looking at UVPD performance across a range of precursor charge states from several studies helps provide a composite picture of the performance of the two methods. Note, differences in AGC targets, instrument platforms, and other experimental parameters make comparisons of product ion signal, etc. less than straight-forward, but differences in product ion types are still interesting to compare. Product ion signal is spread amongst six main product ion channels in UVPD, whereas the major types of AI-ETD product ions are c- and z ●-type. Both methods offer benefits; AI-ETD keeps product ion signal in relatively few channels, avoiding dilution of signal amongst many dissociation pathways as mentioned above, whereas the multiple fragment ion types in rich UVPD spectra can provide high confidence in sequence assignment (i.e., multiple product ions can confirm each residue). Note, UVPD data from these three studies include both automated and manual annotation of product ions, including a, a+1, b, c, x, x+1, y, y–1, Y, and z types. AI-ETD data is only from automated annotation of b-, c-, y-, and z-type ions by ProSight Lite, meaning AI-ETD results could slightly improve with further manual annotation to include off-by-one errors. To the best of our knowledge, no UVPD data is available for comparison with proteins larger than carbonic anhydrase, outside of protein complexes, which are clearly not a direct comparison. Regardless, AI-ETD and UVPD appear to provide similar amounts of protein sequence coverage for proteins as large as 30 kDa, which supports results from smaller intact proteins as well [55].
AI-ETD sustains this improved sequence characterization as protein molecular weight increases, and we explored how to improve sequence coverage by using multiple acquisitions of the same precursor with the same dissociation method. Rather than combine spectra from two complementary dissociation methods, we collected three separate raw files for each precursor with each dissociation method. Each data file was deconvoluted individually to get product ions, and product ions from each acquisition were combined. Figure 4a shows the average percent sequence coverage obtained from triplicate acquisitions of HCD, ETD, EThcD, and AI-ETD MS/MS scans for the z = 30 precursor ion of the 39.2 kDa protein aldolase (light blue bars, with error bars showing one standard deviation) and total coverage achieved when combining the three spectra from each dissociation method (dark blue circles). The corresponding average number of matched fragments is shown in Figure 4b. For each of the four methods, the combination of three replicate spectra results in ~15–20 percent increase in coverage over the average obtained for the individual spectra, e.g., 46% versus 40% for AI-ETD. Again, all electron-driven dissociation methods outperform HCD, and AI-ETD provides the greatest average sequence coverage, largest average number of matched fragments, and greatest combined coverage amongst the four methods. Indeed, the results from a single AI-ETD acquisition are approximately equivalent to or more than the sequence coverage from three combined spectra of HCD, ETD, and EThcD. In total, 57% of aldolase’s 362 backbone bonds could be explained when combining AI-ETD and HCD data.
AI-ETD provided the best data for all four precursors of enolase (46.7 kDa), with each being interrogated with two different reaction conditions per dissociation method. In other words, separate spectra that used either a relatively short and relatively long ion–ion reaction time were collected for ETD, EThcD, and AI-ETD, and a relatively low and high normalized collision energy were used for HCD. The reaction times and collision energies used varied for each charge state, but the same two ion–ion reaction times were used for ETD, EThcD, and AI-ETD fragmentation of a given precursor ion charge state. Figure 5a displays the outcome of these experiments, showing the sequence coverage resulting from the short reaction time (or low HCD collision energy) in light blue bars and the long reaction time (or high collision energy) in dark blue bars. The gray lines above each pair shows the total sequence when combining the spectra from the two conditions for each fragmentation method. Note, the full MS1 spectrum of enolase (in addition to aldolase and BSA) is provided in Supplemental Figure 2, showing the charge state envelope and the precursor ion charge states selected for dissociation in these experiments.
Several interesting trends arise from these data, perhaps most strikingly that AI-ETD at the longer reaction time (i.e., a single condition) generated more sequence coverage than the combination of two reaction conditions of HCD, ETD, and EThcD for all precursors except z = 52 (where it still provided the greatest combined coverage). The benefit of slightly longer reaction times have been previously reported for the high capacity ETD accumulation scheme, which may explain why longer reaction times generally provided better data [58]. Also, the diminishing benefit of EThcD over ETD is juxtaposed with the consistent boost in performance with AI-ETD. Figure 5b provides the total number of matched fragments from the combined reaction conditions for each precursor. As expected, HCD performance increased from high to low charge states, ETD performance decreased from high to low charge states, and AI-ETD provided consistent performance for all four precursors. Figure 5c displays a sequence coverage map for enolase for the combination of AI-ETD and HCD data from the z = 40 precursor for 54% coverage of the 46.7 kDa protein.
Figure 6 compares ETD and AI-ETD dissociation of z = 60 (panel a) and z = 70 (panel b) of BSA, which has a molecular weight of ~66.8 kDa after reduction of its disulfide bonds and carbamidomethylation of its cysteines. Ten different ion–ion reaction times ranging from 4 to 40 ms were used for both ETD and AI-ETD for each of the precursor ions. Characterization generally improved with increasing reaction time although longer times provided diminishing returns, especially for ETD. When combining fragments from all 10 acquisitions, each condition contributed unique sequence-informative ions, indicating the different reaction times can access somewhat different information (similar to the trends seen with enolase). More importantly, AI-ETD provided a boost in sequence coverage over ETD for each measurement, especially at longer reaction times, and provided the best results when combining data from all conditions for either precursor. Although this trend follows that of the other protein data in this work, it was not necessarily an expected outcome when considering the high charge states of the precursor ions. When combining data from both charge states, which is another strategy often employed when characterizing larger intact proteins, AI-ETD generates 25% sequence coverage to ETD’s 19% (Figure 6c). Note, a summary of results and methods for achieving the best coverage of all four protein standards in this study is available in Supplemental Table 1.
Conclusions
This work describes the first application of AI-ETD to larger protein precursor ions (30–70 kDa), a molecular weight range where an analysis technology gap still exists. We show that AI-ETD provided the greatest sequence coverage over HCD, ETD, and EThcD for a variety of precursor ion charge states spanning the m/z range for carbonic anhydrase, aldolase, enolase, and bovine serum albumin (BSA). AI-ETD not only improved performance over ETD for low-charge density precursor ions, but it also maintained boosted performance for the higher charge states of each protein. This was not the trend for the other supplemental activation method explored in this work, EThcD, which proved useful for low charge states of the smaller proteins but did not greatly increase coverage for higher charge states. Beyond comparing dissociation methods, we also demonstrated how different data acquisition strategies to combine spectra can affect larger protein ion characterization with AI-ETD in concert with other fragmentation methods. Overall, AI-ETD produced the most robust and consistent fragmentation for all precursor ions investigated here, demonstrating its suitability as a universal fragmentation method for top-down proteomics, both less than and greater than 30 kDa. Furthermore, this work highlights the established value of ETD in general for the characterization of intact protein ions, as it outperforms HCD in nearly all instances.
Not surprisingly, the gains in sequence coverage and overall protein characterization diminished as protein size increased. Several factors contribute to this, including challenges in controlling ion–ion reactions for very highly charge precursor ions to preserve highly charged fragments and in successfully deconvoluting congested spectra that arise from dissociation of large biomolecules. Several groups have described the use of proton transfer reactions, ion parking, and combinations thereof to address these challenges and improve the characterization of intact protein ions [60,61,62,63], and we foresee AI-ETD being a powerful addition to these approaches. This can be especially valuable for dissociation of intact antibodies (~150 kDa), where ETD has been critical for top-down characterization, but sequence coverages remain moderate and success requires extensive spectral averaging in addition to analyses of several charge states [47, 64, 65]. A recent study discussed the benefits of EThcD for improved intact antibody fragmentation [66], leading us to suppose that AI-ETD could provide even larger boosts. Finally, as the newest instrumentation extends the mass range at which tandem MS can be effectively performed [67], AI-ETD is well-suited to be a useful platform for dissociating larger proteins and potentially protein complexes [68], offering more extensive information than can be generated by other dissociation methods. In all, AI-ETD provides an exciting avenue forward as top-down proteomics continues to expand investigations to proteins with larger and larger molecular weights.
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Acknowledgments
The authors gratefully acknowledge support from Thermo Fisher Scientific and NIH grants R35 GM118110 and R21 GM118341 (to J.J.C.). N.M.R. was funded through a NIH Predoctoral to Postdoctoral Transition Award (F99 CA212454). Thank you to John Syka, Chris Mullen, Will McGee, and Jim Stephenson for helpful discussions.
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Riley, N.M., Westphall, M.S. & Coon, J.J. Sequencing Larger Intact Proteins (30-70 kDa) with Activated Ion Electron Transfer Dissociation. J. Am. Soc. Mass Spectrom. 29, 140–149 (2018). https://doi.org/10.1007/s13361-017-1808-7
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DOI: https://doi.org/10.1007/s13361-017-1808-7