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BioSAXS special applications Martin A. Schroer EMBL Hamburg - PowerPoint PPT Presentation

BioSAXS special applications Martin A. Schroer EMBL Hamburg Examples for bioSAXS experiments Disclaimer Might not work for all samples Might not make sense for all samples You will likely need more sample solution however


  1. BioSAXS – special applications Martin A. Schroer EMBL Hamburg

  2. Examples for bioSAXS experiments Disclaimer • Might not work for all samples • Might not make sense for all samples • You will likely need more sample solution however • can give fundamental new insights • In situ • Time-resolved • … • demand a synchrotron source Contact the beamline scientists! • Photon flux: weak signals, temporal resolution • Small beam sizes: spatial resolution • Energy tunability: Penetration 2

  3. Types of sample environments Robotic sample changer • Capillary holder Microfluidics (e.g. for THz) • Temperature cell • in vacuum capillary • continuous flow • Cryo chamber (P12) • High pressure cells • Rheological cells • Heating stages • User setups • … SEC-SAXS/MALS Laser excitation Stopped Flow • Online purification and 28/02/2020 3 detection system

  4. Non-standard bioSAXS • Biological macromolecules under external perturbations • Heat • Pressure • Shear stress • Laser light • THz-radiation • Examples for hierarchial samples • Radiation damage • Static • Time-resolved 4

  5. In air operation In vacuum: • Quarz capillary • Removing in vacuum capillary / sample changer • Two sealing windows + BSA + buffer  Air gap + buffer • Place sample cell  Higher X-ray absorption by air  Higher background signal (air + windows + sample cell ) In air Try to reduce the air gap as • Polystyrene cell much as possible! • Air • Kapton windows Use proper window material! + BSA + buffer + buffer 5

  6. Heating stages (at P12) Sample changer temperature range: • 7 – 40 ° C • Keep samples stored at different T Temperature controlled capillary holder • Peltier element • Quartz capillaries • different T range • fast T changes User setup • highly viscous samples • e.g. Linkam heating stage • tricky samples (toxic, corrosive, dirty,..) • Apolar solvent • for non-liquid samples 6

  7. Temperature SAXS studies • Unfolding of proteins • Gelation processes • Coil-to-globule transition (biopolymers) • Phase transitions in lipids, liquid crystals • … Example: • Biological relevant lipids • T-induced melting of lamellar structures F. A. Facchini et al. J. Med. Chem. 61, 2895 (2018). 7

  8. High Pressure SAXS Allows to study protein stability • (pressure-) unfolded state smaller volume than folded state (~ 1% effect) • Pressure 1 – 7 kbar : effect on non-covalent bonds: Changes of the tertiary structure • Pressure > 10 kbar : effect on covalent bonds: changes of the secondary structures Need High pressure sample cells • Pressure range: 1 bar – 4....7 kbar • X-ray windows: two flat diamonds -> Higher X-ray energy! • Pressurizing medium: water 8 27/05/2020 C. Krywka et al. , ChemPhysChem 9 2809 (2008).

  9. HP SAXS – SNase • 149 amino acids, M w = 16.8 kDa • Globular protein • No disulfidec bonds -> destabilized • Standard protein for high pressure studies High pressure effects • Decrease of I(0) ⇒ reduced constrast as water gets compressed • Increase of radius of gyration ⇒ unfolding Guinier plot G. Panick et al. , J. Mol. Biol. 275, 389 (1998). 9

  10. SNase - (de-)stabilization by cosolvents C. Krywka et al. , ChemPhysChem 9 2809 (2008). Cosolvents can change the pressure – effect • Kosmotropic: stabilizing • Chaotropic: destabilizing Urea p [bar] • destabilizes proteins TMAO • Stabilizes, counteracts urea • Concentration in fishes increases with sea depth p [bar]  Recently more studies (several protein, tRNA, microtubuli) but still more to be explored: terra incognita 10

  11. Rheo-SAXS: Effect on shear • Shear can align or disrupt molecules; is present in joints and blood flow Hyaluronan: 750 kDa • Hyaluronan is a biopolymer and essential part of the extracelluar matrix (joints) 0 - 1500 1/s  Rheo-SAXS: Hyaluronan chain network gets more ordered 11 D.C.F. Wieland et al. , J. Syn. Rad. 24, 646 (2017).

  12. Light-induced reactions Light can induce different types of reactions • 360 – 500 nm:  Structural changes of photosensitive proteins  Opening of caged compounds • Infra red (1440 nm):  Temperature jump by fast heating of water Example: • Caged ATP released after laser pulse • ATP induces dimerization of NBD • TR-SAXS/WAXS Tidow group (Hamburg) @ ID09, ESRF 12 I. Josts et al. IUCrJ 5, 667 (2018).

  13. P12 – laser system To fibre • Tuneable Nd:YAG – laser ( Ekspla , Lithuania) Direct • Wave lengths: • 335 – 500 nm & 1065 – 2500 nm (fibre port; to P12 hutch experiments) • Repetiton rate: 10 Hz • Pulse length: 6 ns Energy per pulse [mJ] 13

  14. Studying the effect of THz on proteins THz radiation • Electromagnetic radiation • Can induce large molecular vibrations (collective) / low in energy • Strong absorption in water • Non-ionizing but thermal/ athermal effects -> possible risks are discussed in literature 14 L. Wei et al. Frontiers in Laboratory Medicine (2019).

  15. THz-excitation of proteins Fröhlich‘s prediction • THz-radiation can excite collective motions within biological macromolecules by coupling to their dipole moment ( Fröhlich condensation ) Such collective vibrations ( normal modes ) may lead to long-range conformational changes . Such changes can be probed by SAXS.  THz excitation & SAXS probe 15 A. Panjkovich, D.I. Svergun. PCCP 18, 5707 (2016).

  16. THz-SAXS - Experiment Such a noval type of experiment needs • THz sources (cw + pulsed) -> Excite the sample • Dedicated microfluidic cell -> small channel width Setup I • Sample delievery system Setup II • Small, asymmetric X-ray beam (80 x 120 µm 2 ) • Precise positioning (sub-micron) (hexapod) • Synchronization (data collection) M. Roessle (TH Lübeck) 16 G. Katona (U Gothenburg)

  17. THz-SAXS - microfluidic cell Combined THz-SAXS measurements demand dedicated sample environment Microfluidic chips: • • Flowing of sample → reduce radiation damage • Transparent for THz → enough sample excitation • Narrow channel (500 µm) as THz absorption in water is strong → enough sample excitation • Low X-ray background → record SAXS signal  3D printed Polystyrene cell M. Roessle (TH Lübeck) 17 S. Schewa, et al., submitted

  18. Setup installed at P12 • THz beam passes set of mirrors THz • THz can be detected by receveiver • THz beam & X-ray beam are perpendicular X-ray  The same stop of the sample is illuminated 18

  19. SAXS on cells • Recently, SAXS / USAXS studies have been performed on cells • Example: E. coli modelled with a geometrical model • Application in screening studies for different antibiotics E.F Semeraro et al. , IUCrJ 4, 751 (2017). 19 A.R. v. Gundlach et al. , BBA - Biomembranes 1858, 918 (2016).

  20. Scanning SAXS • Scan samples with a small X-ray beam  Real space maps of scattering intensity • Examples: • SAXS from the inside of cells • Structure of bone (orientation of hydroxyapatite crystals) B. Weinhausen et al. , Phys. Rev. Lett. 112, 088102 (2014). 20 16/03/2018 D.C.F. Wieland et al. , Acta Biomaterialia 25, 339 (2015).

  21. SAXS tensor tomography • Method to study anisotropically oriented nanostructures at 3D spatial resolution • Example: Orientation of collagen fibrils within a trabecular bone 21 M. Liebi et al. , Nature 527, 349 (2015).

  22. Radiation damage in protein solutions 2 H 2 O + X-ray → H 3 O + + • OH + e - • Mechanism of radiation damage: aq Radiolysis of water (99 % of sample volume) • + - OH e - aq + O 2 → HO 2 → radical formation S.D. Maleknia et al., Anal. Biochem. → interactions with solvent accessible sites 289 , 103 (2001). → formation of large aggregates For SAXS: Aggregates spoil signal of undamaged proteins C.M. Jeffries et al., J. Syn. Rad. 22 ,  Radiation damage limits data collection of biological samples 273 (2015). 22

  23. Reducing radiation damage Coflow N. Kirby et al., Acta Problem for SAXS: Damage not ( easy ) predictable Cryst. D 72 , 1254 (2016).  Different schemes to reduce the effect of radiation damage Cryo-cooling Beam attenuation S.P. Meisburger et al., Biophys. • J. 104 , 227 (2013). Addition of „scavenger“ or stabilizer molecules • (DTT, ascorbic acid; glycerol) High flux Continous sample flow • Coflow • • Cryo-cooling • Outrunning radiation damage (High flux) Cell geometry • Sample cell geometry M.A.Schroer et al. , J. Synchrotron Rad. 25 , 1113 (2018) 23

  24. TR BioSAXS Proteins are scattering weakly • need more flux • possible to follow a changing signal However: • Radiation damage is harder to determine: • Data comparsion does not work How to deal with this? 24

  25. Example: Stopped Flow TR-SAXS • Reaction of MsbA Nucleotide binding domain with ATP • Rapid mixing • 35 ms frames collected • Expected: Monomer – dimer transition H. Tidow 25 Josts et al, Structure 28, 348 (2020).

  26. • Start reaction and directly probe  Continuous change of Rg 26

  27. • Start reaction and directly probe  Continuous change of Rg • Start reaction, wait (delay time), then probe  Continuous change of Rg But NOT overlapping  Radiation Damage 27

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