Leonhard H.
Urner
*abc,
Maiko
Schulze
a,
Yasmine B.
Maier
a,
Waldemar
Hoffmann
ab,
Stephan
Warnke
b,
Idlir
Liko
c,
Kristin
Folmert
a,
Christian
Manz
a,
Carol V.
Robinson
c,
Rainer
Haag
a and
Kevin
Pagel
*ab
aInstitute of Chemistry and Biochemistry, Freie Universität Berlin, Arnimallee 22, 14195 Berlin, Germany. E-mail: leonhard.urner@fu-berlin.de
bDepartment of Molecular Physics, Fritz Haber Institute of the Max Planck Society, Faradayweg 4-6, 14195 Berlin, Germany. E-mail: kevin.pagel@fu-berlin.de
cPhysical and Theoretical Chemistry Laboratory, University of Oxford, South Parks Road, OX13QZ Oxford, UK
First published on 13th March 2020
Mass spectrometry enables the in-depth structural elucidation of membrane protein complexes, which is of great interest in structural biology and drug discovery. Recent breakthroughs in this field revealed the need for design rules that allow fine-tuning the properties of detergents in solution and gas phase. Desirable features include protein charge reduction, because it helps to preserve native features of protein complexes during transfer from solution into the vacuum of a mass spectrometer. Addressing this challenge, we here present the first systematic gas-phase study of azobenzene detergents. The utility of gas-phase techniques for monitoring light-driven changes of isomer ratios and molecular properties are investigated in detail. This leads to the first azobenzene detergent that enables the native mass spectrometry analysis of membrane proteins and whose charge-reducing properties can be tuned by irradiation with light. More broadly, the presented work outlines new avenues for the high-throughput characterization of supramolecular systems and opens a new design strategy for detergents in membrane protein research.
Generally, detergents are of limited use when the intended application requires their properties to be dynamically altered during the application. To enable such remote control, detergents are often modified with azobenzene, which consists of two phenyl rings that are held together by a NN bond.9 Azobenzene exists either in a thermodynamically more stable trans or a metastable cis form.10 The light-driven interconversion between both isomers effectively changes their structure,10 dipole,11 and basicity,12,13 which has driven the development of photoresponsive materials.14–16 Research on azobenzene detergents has been focused on photoresponsive surface coatings,17–20 catalysis systems,21 and supramolecular aggregates.22–27 The utility of anionic 4-hexylphenylazosulfonate for denaturing top-down proteomics has been outlined very recently.28 As ionic detergents commonly denature membrane proteins more than non-ionic detergents,29 this inspired us to investigate whether non-ionic azobenzene detergents can be used for the non-denaturing structural analysis of membrane proteins.
A ubiquitous challenge for structure–property analysis of azobenzene detergents is the characterization of their individual isomers. Condensed-phase techniques average the results obtained from the entire population of species within a sample. The light-driven isomerization is almost never quantitative30 rendering the unambiguous analysis of individual isomers difficult. Ion mobility-mass spectrometry (IM-MS) can circumvent this challenge, because it allows to characterize individual species in the presence of many others.31 Briefly, ions are separated according to the time required to pass a cell that is filled with a neutral buffer gas. This drift time depends on the mass, charge, and overall shape of an ion, which enables the separation of isomers.24,32–35 To gain further insights into the molecular structure, drift times are typically converted to collisional cross-section (CCS) values. They represent the ion's rotationally averaged cross section interacting with the buffer gas. CCS values are independent from instrumental parameters and can be derived from theoretical calculations.36,37 Comparing experimental and theoretical CCS values provides insights into the overall structure of isomers.36 While IM-MS is sensitive to the ions' overall shape, infrared multiple photon dissociation (IRMPD) spectroscopy on IM-selected ions can provide additional details about the ions' molecular structure.36,38 In IRMPD, ions are dissociated in a mass spectrometer in a wavelength dependent manner.
Here, we systematically investigate the molecular properties of azobenzene detergents and their utility for protein mass spectrometry. We focus on two detergent families: oligoglycerol bola-type detergents (OGBAs) and oligoglycerol detergents (OGDs, Fig. 1). We explore the utility of gas-phase techniques for quantifying their relative cis/trans ratios from solution and analyse how the molecular shape of these detergents is affected by (i) their isomeric state, (ii) general architecture, and (iii) structure of the hydrophobic backbone. By taking advantage of these findings we explore the utility of non-ionic azobenzene OGDs for the native MS analysis of membrane proteins.
The relative intensity obtained from doubly protonated cis3 [M + 2H]2+ at the Synapt is about 60% lower compared to solution (Fig. 2). This indicates that cis to trans isomerization occurred between nanoelectrospray ionisation (nESI) and IM analysis, which is very likely a result of the non-continuous pressure profile of the Synapt instrument (Fig. S2, ESI†). In Synapts, ions traverse a high-vacuum region between the ion source and IM cell. Subsequent transfer and injection of the ions into the IM cell is accompanied by an increase in pressure of about four orders of magnitude. This causes collisional heating of the ions and is likely to induce cis to trans conversion prior the IM separation.48,49 In comparison, instrument pressure is continuously decreasing between the ion source and IM cell of typical DT instruments (Fig. S2, ESI†), thus leading to a softer ion transmission50 and a higher relative intensity of doubly protonated cis (Fig. 2). The isomer ratio obtained from DT analysis of doubly protonated cis matches with data obtained from solution (Fig. 2). In addition, our results suggest that the effect of collisional heating on the cis/trans ratio is supported by protonation of ions during nESI. Protonation of the cis NN bond lowers the activation energy for the thermal cis to trans isomerization,46 which serves an additional explanation for the reduced relative intensity of doubly protonated cis under harsh instrument conditions (Fig. 2).
In contrast, relative intensities of doubly sodiated cis3 [M + 2Na]2+ were about 11% lower compared to solution, irrespective of the IM-MS instrument type (Fig. 2). In comparison to protons, sodium ions are more likely located at the crown ether-like head groups.7 The slightly reduced relative intensity of doubly sodiated cis3 might have two reasons: first, charge repulsion between sodiated head groups could lower the thermal stability of cis. Second, isomer ratios obtained from IM-MS may also be affected by the ionization efficiency of individual isomers and ion adducts.
In summary, only the DT IM-MS analysis of doubly protonated 3 revealed a cis/trans ratio that matches with solution data (Fig. 2, Table S1, ESI†). Further tests on OGDs 6, 8, and 10 led to comparable isomer ratios only in case of sodiated ions (Table S2, ESI†). This leads us to the conclusion that the ability to quantify cis/trans ratios from solution by IM-MS depends on both instrument conditions and properties of the investigated species. Our data underline that IM-MS enables the quantification of relative cis/trans ratios from solution. However, IM-MS may not be used as stand-alone technique. Reference data from solution are needed for the identification of IM-MS instrument conditions that deliver comparable results.
The CCS values obtained from singly charged cis and trans OGBAs 1–5 are similar, irrespective of the size of the hydrophobic backbone (Fig. 3). Charge interactions, either attractive or repulsive, are enhanced in the absence of solvent.51 For singly charged OGBAs, this causes very likely intramolecular interactions between the triglycerol head groups and forces the detergent into a more compact conformation. According to this scenario, distinct structural features of cis and trans are poorly reflected in the overall shape of the detergents (Fig. 3). In line with this explanation, two well-distinguishable CCS values are obtained for doubly charged ions of cis and trans1, 2, 3, and 4 (Fig. 3). Here, charge-repulsive interactions prevent the head groups from intramolecular interactions and two distinguishable conformations are obtained (Fig. 3). Conversely, CCS values obtained from cis and trans5 are similar, irrespective of the charge state (Fig. 3). We conclude that increasing the size of the alkyl spacers reduces the impact of isomeric state and charge state on the overall shape of OGBAs (Fig. 3). This might have two reasons: first, elongating the alkyl spacers lowers the relative proportion of azobenzene in the overall detergent structure. Second, long alkyl spacers facilitate more conformational freedom.27
In comparison to OGBAs, only one head group is present in OGDs rendering a collapse of the gas-phase structure unlikely. As a consequence, clearly separated CCS values are obtained from singly charged cis and trans OGDs 6–10 (Fig. 3). This underlines that the ability to separate cis and trans by IM-MS depends not only on the charge state but also on the general architecture of the investigated species. Again, differences in CCS between cis and trans OGDs become smaller with increasing size of the hydrophobic backbone (Fig. S4, ESI†), thus indicating that this correlation can be extrapolated to other detergent classes. The length of alkyl spacers affects the polarity and shape of detergents.27,52,53 Our data underline that IM-MS allows us to analyse in addition how the overall shape of azobenzene detergents is affected by the interplay between (i) isomeric state, (ii) general molecular architecture, and (iii) size and flexibility of the hydrophobic backbone; all of which determine the aggregation behaviour of azobenzene detergents.23,24,27,42 In light of these results we anticipate that IM-MS could be used as a diagnostic tool that helps to tune the photo-switchable properties of supramolecular systems in the future.
Similar theoretical CCS values were obtained from simulated conformers of trans1 (208 ± 2) Å2 and cis1 (206 ± 2) Å2 in which both head groups stick together (Fig. S5, ESI†). However, the differences in theoretical CCS values are similar within their errors rendering a clear explanation of the experimental result by molecular dynamics simulations difficult.
Therefore, we investigated singly protonated ions of 1 by IRMPD spectroscopy after they have passed the IM cell (Fig. S6, ESI†). The spectrum obtained from singly protonated trans1 shows multiple features: amide I band (∼1700 cm−1), aromatic backbone (∼1600 cm−1), amide II band (∼1500 cm−1), CNN band (1340 cm−1), and overlapping bands from the head groups (<1300 cm−1, Fig. 4).54,56,57 The structure of trans1 offers multiple protonation sites, including the head groups, carbonyl groups, triazoles, and the NN bond. The obtained IR bands match with those of unprotonated carbonyl and triazole groups and provide no evidence that protonation of the trans N
N group occurred.54,56,57 This leads to the conclusion that the triglycerol head groups are the main protonation sites of trans1 during nESI. Surprisingly, the ether and hydroxyl groups of the triglycerol head groups are associated with lower gas-phase basicity values than other building blocks (Table S3, ESI†). This indicates that the preferred protonation site of a molecule depends not only on the gas-phase basicity but also on the number and accessibility of its functional groups.58
The IRMPD spectrum obtained after irradiation of the sample solution at 366 nm represents an average of a singly protonated cis/trans mixture, because the light-driven isomerization in solution is not quantitative and protonated isomers of 1 are not separable by IM (Fig. S5, ESI†). However, an additional IR band appeared at 1430 cm−1 after irradiation at 366 nm (Fig. 4). The obtained wavenumber is lower than values reported for the protonated NN bond of unsubstituted cis azobenzene (1478–1515 cm−1).54 This is expected since it is known that the electron-donating alkoxy groups of azobenzene lower the double-bond character of the protonated N
N bond (Fig. S7, ESI†).54,56 The appearance of the new band at 1430 cm−1 together with changes in relative intensities of head group vibrations (<1200 cm−1) indicate that the average protonation site of 1 changed to the N
N bond after irradiation at 366 nm. Taken together, our data underline that protonated cis1 retains its double bond configuration during nESI and IM analysis under the experimental conditions employed.
To address this question, we purified the trimeric ammonia channel (AmtB) from cell membranes of E. coli using n-dodecyl-β-D-maltoside (DDM) and exchanged the detergent environment from DDM to trans OGD 6 using size-exclusion chromatography. The so-obtained membrane protein solution was stable over multiple freeze–thaw cycles, before and after irradiation at 366 nm, which confirms the utility of trans6 and its cis/trans mixture to solubilize and stabilize membrane proteins. To investigate if the native quaternary structure of AmtB was preserved upon detergent exchange, we analysed the samples by native MS. The mass spectra obtained before and after irradiation at 366 nm revealed AmtB in its native trimeric state together with gas-phase dissociation products, such as monomers and dimers.8 This shows that trans6 and its cis/trans mixture cannot only solubilize but also preserve the native oligomeric state of AmtB. The most abundant charge state of AmtB obtained from the MS analysis with trans6 (21+) is similar to that obtained from DDM (22+), which is classified as a non-charge-reducing detergent (Fig. 5).6 Upon irradiation at 366 nm, a bimodal charge state distribution appeared and the most abundant charge state was shifted to higher m/z values (18+, Fig. 5).
While the shift in the most abundant charge state indicates that cis6 is more charge-reducing than trans6, the bimodal charge state distribution also indicates that AmtB partially unfolded.60 To investigate if the protein unfolded in solution, we analysed the secondary structure of AmtB by circular dichroism (CD) spectroscopy. We obtained a similar alpha-helical content in DDM and 6, before and after irradiation at 366 nm (Fig. S8, ESI†). We conclude that trans6 as well as its cis/trans mixture can preserve the native fold of AmtB in solution. The bimodal charge state distribution obtained upon irradiation at 366 nm reflects therefore likely partial protein unfolding during nESI.60
Detergents are in many ways important for the native MS analysis of membrane proteins as they can protect the native structure in solution and during the nESI process.6,8,59 The detergent concentration used for solubilising membrane proteins is often adjusted to a multiple of the detergents' critical aggregation concentration (cac).8 Attempts to solubilise AmtB with concentrations below the cac of trans6 led to protein precipitation, thus underlining that at least concentrations close to the cac are needed to stabilize AmtB in aqueous buffer. The different charge state distributions obtained for AmtB, before and after irradiation at 366 nm, motivated us to further investigate the properties of the detergent micelles in solution. Interestingly, similar cac values were obtained for 6, before and after irradiation at 366 nm (Fig. S9, ESI†). The diffusion coefficients of the aggregates were similar and in the same order of magnitude as values reported from other micelle-forming [G2] OGDs (Fig. S9, ESI†).41 This indicates that trans6 as well as its cis/trans mixture are capable of forming micelles. While investigating the molecular properties of our azobenzene detergents we found that the trans to cis isomerization is affecting the geometry and polarity of the hydrophobic tail (Fig. 3 and 4). Micelles formed by the cis/trans mixtures are more heterogeneous than those solely formed by trans azobenzene detergents.23 It is very likely that the bent and more polar cis form disturbs the packing of the micelles.23 In this way, cis6 could lower the efficiency of the micelle in shielding the hydrophobic protein surface and facilitate, for example, partial protein unfolding during nESI.
To gain more insights into the charge-reducing properties of 6, we extended our studies on the soluble protein β-lactoglobulin (BLG). This protein contains an amphiphilic pocket that is capable of forming non-covalent complexes with detergents.7 Unlike membrane proteins, BLG is not encapsulated in micelles and serves as an ideal model system to study the impact of individual functional groups of detergents on the ability to reduce the charge of protein ions in the gas phase.7 For this purpose, OGDs and BLG were mixed in solution and analysed by nESI-MS using a modified Ultima high-mass quadrupole time-of-flight mass spectrometer (for further details see ESI†). Subsequently, the gas-phase dissociation behaviour of protein–detergent complexes (PDCs) formed by 6 and BLG was analysed by tandem mass spectrometry (MS/MS). Closer analysis of the dissociation products revealed how the isomerization of azobenzene mediates the ability of 6 to remove protons from protein ions within the vacuum of a mass spectrometer.
Mass spectra obtained from equimolar mixtures of OGD 6 and BLG show a narrow protein charge state distribution with charge states ranging from 6+ to 10+ (Fig. S10, ESI†). To take into account in our analysis that the dissociation behaviour of non-covalent protein complexes varies significantly with the protein charge state,61 MS/MS experiments were focused on the most abundant protein charge state 8+ (Fig. 5). Upon dissociation of fully protonated PDCs, three new ion populations appeared. They could be assigned as protonated detergent ions and BLG of two different charge states (8+ and 7+, Fig. 5). Before irradiation of the sample solution, the most intense protein charge state belongs to non-charge reduced BLG (8+, Fig. 5). After irradiation, the most intense protein charge state belongs to charge-reduced BLG (7+, Fig. 5). This confirms that the increase in NN bond basicity of azobenzene during trans to cis isomerization affects the detergent's propensity to pick up a charge from the protein ion during PDC dissociation.
To analyse underlying changes in basicity of azobenzene, MS/MS experiments were repeated with OGDs in which azobenzene was substituted for linker groups with different gas-phase basicity values, such as ether (794 kJ mol−1), amide (820 kJ mol−1), and triazole (925 kJ mol−1, Fig. S11,† Table S3, ESI†).7,62,63 The fraction of charge-reduced BLG (%) obtained upon PDC dissociation was plotted against the gas-phase basicity values of the linker groups and the data were fitted to a linear function. An extrapolation to the gas-phase basicity values of 6 indicates that its average gas-phase basicity went up by 60 kJ mol−1 after irradiation of the sample solution at 366 nm (Fig. S12†). This implies that optimizing the isomerization yields and gas-phase basicity values of cis can maximize protein charge reduction. To the best of our knowledge, OGD 6 presents the first example of an azobenzene detergent that enables the native MS analysis of a membrane protein complex and whose charge-reducing properties can be changed by irradiation with light.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d0sc01022g |
This journal is © The Royal Society of Chemistry 2020 |