Small molecules are known to stabilize membrane proteins and to modulate their function and oligomeric state, but such interactions are often hard to precisely define. Here we develop and apply a high-resolution, Orbitrap mass spectrometry–based method for analyzing intact membrane protein–ligand complexes. Using this platform, we resolve the complexity of multiple binding events, quantify small molecule binding and reveal selectivity for endogenous lipids that differ only in acyl chain length.
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The authors would like to thank L. Feng and W. Frommer (Stanford School of Medicine) for the semiSWEET plasmid. This work has benefited from the expertise of the Protein & Nucleic Acid Chemistry Facility, Department of Biochemistry, University of Cambridge, UK for quantification of the OBS1 peptide. We would also like to thank A. Baldwin for help with dissociation constant calculations. K.G. is supported by a Royal Commission for the Exhibition of 1851 Fellowship and a Junior Research Fellowship at St Catherine's College, Oxford. J.A.C.D. is supported by an Engineering and Physical Sciences Research Council studentship held at the Life Sciences Interface Doctoral Training Centre. M.T.M. and J.T.S.H. are funded by program grant G1000819 (C.V.R.) from the UK Medical Research Council. J.G. is funded by a European Research Council Investigator Award (IMPRESSS, grant no. 268851) (C.V.R.). C.V.R. is supported by a Royal Society Research Professorship and a Wellcome Trust Senior Investigator Award (grant no. 104633/Z/14/Z). C.V.R. and C.K. acknowledge BBSRC for funding (BB/L021234/1) (C.K.).
E.D., M.B. and A.M. are employees of Thermo Fisher Scientific, the manufacturer of the Q Exactive instrument used in this research.
Integrated supplementary information
Supplementary Figure 1 Schematic of modified Q Exactive instrument with major modifications indicated.
Further details are provided in the Online Methods section.
Supplementary Figure 2 Gradual release of the AmtB trimer from C8E4 micelle upon increasing collision energy in the HCD cell.
The protein is completely released by accelerating ions into the HCD cell with 100 V and detergent continues to be stripped without charge state broadening up to 200 V.
Supplementary Figure 3 Spectra of pentameric ligand-gated ion channel ELIC acquired at different HCD pressures.
Pressures as measured with UHV pressure gauge (mbar). Due to the location of the gauge to calculate actual pressure in the HCD cell a scaling factor must be applied to the values from the read back stated here. (a) 6×10-10, (b) 9.09×10-10, (c) 1.35×10-9, (d) 1.76×10-9, (e) 2.43×10-9. At low pressure (a) only monomeric ELIC is transmitted. This probably because the collisional cooling effect in the HCD cell is insufficient to retain the more massive, higher order oligomers. As the pressure is increased b-c) the transmission of higher mass species is improved and the familiar ELIC spectrum of pentamer accompanied by stripped tetramer and monomer is observed. At higher pressures d-e) dissociation appears to be reduced until only the intact pentamer is observed.
Supplementary Figure 4 Representative data set for titration of OBS1 peptide with OmpF trimer at different concentrations of peptide ligand.
Concentration of OmpF trimer in each case is 8.9 μM.
(a) Overall binding of OBS1 peptide to OmpF and fit to a single site binding model as described previously30 giving best fit KD of 0.69 mM (0.64 ± 0.14 mM after 1,000 bootstraps). (b) Individual microscopic site KD’s for successive binding events. Microscopic KDs for a 1 protein, 3 ligand, 3 binding sites per protein model were obtained by testing different fit models (free, single KD) choosing the best model based on an F-test. This was consistently the free model which allows each binding event to have a different KD. All data was processed using the data collector module of the UniDec software which is available for download at http://unidec.chem.ox.ac.uk 16. (c) Distribution of errors for calculation of microscopic KDs after 1000 bootstraps.
(a) Mass spectrum of P-gp. The increased resolution now reveals three major proteoforms labelled P1, P2 and P3 in contrast to previous results4. (b) Binding of cardiolipin 14:0 (CDL 14:0, blue square) to P-gp Binding is observed on all three preforms. (c) Binding of drug Cyclosporin A (CsA, red circle) to P-gp. Binding is again observed on all three preforms. (d) Concomitant binding of both drug and lipid. Insets are zooms of single charge states showing up to two binding events.
Supplementary Figure 7 Binding of individual lipids of different chain lengths and degrees of unsaturation to OmpF trimer
(a) DMPG, (b) DPPG, (c) POPG. The mass spectrum of OmpF trimer binding to POPG allows a good estimation of the dynamic range of such measurements with clear peaks discernible over 1.5 to nearly 2 orders of magnitude.
(a) MS Full scan TIC of total lipid extract analyzed by RP LC-MS. (b) Summed MS scans corresponding to the region where cardiolipin elutes showing the distribution of CDL with different chain lengths. (c) MS/MS spectrum of the peak at 1375.97 m/z identifying the lipid as 66:2 CDL by similarity to reported CDL spectra (Hsu, F.-F. et al., Journal of the American Society for MS 16, 491-504 (2005).)
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Gault, J., Donlan, J., Liko, I. et al. High-resolution mass spectrometry of small molecules bound to membrane proteins. Nat Methods 13, 333–336 (2016). https://doi.org/10.1038/nmeth.3771
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