Recent Advances in Protein Powder Diffraction R.B. Von Dreele, XSD/IPNS Argonne National Laboratory, USA “Reaching for High Resolution in Protein Powder.

Slides:



Advertisements
Similar presentations
Reciprocal Space Learning outcomes
Advertisements

SOMO Workshop, 20th Intl AUC Conference, San Antonio, TEXAS, 25th - 30th March, 2012 Small-Angle X-ray scattering P. Vachette (IBBMC, CNRS UMR 8619 & Université.
IX. X-ray diffraction 9-1. Production of X-ray Vacuum, thermionic emission, high voltage,
An introduction to the Rietveld method Angus P. Wilkinson School of Chemistry and Biochemistry Georgia Institute of Technology.
Focusing monochromators/analyzers Asymmetric diffraction geometry of the monochromator Dispersive double crystal monochromator Two wavelength sandwich.
Do it with electrons ! II.
Crystal diffraction Laue Nobel prize Max von Laue
Plan : lattices Characterization of thin films and bulk materials using x-ray and electron scattering V. Pierron-Bohnes IPCMS-GEMME, BP 43, 23 rue du Loess,
Introduction to protein x-ray crystallography. Electromagnetic waves E- electromagnetic field strength A- amplitude  - angular velocity - frequency.
1. Detector 2. Crystal diffraction conditions
Laue Photography Mathematics Structures time-resolved crystallography neutron crystallography electron crystallography.
CHAPTER 3: CRYSTAL STRUCTURES X-Ray Diffraction (XRD)
X-Ray Experiment Presenter: Xu Luo Dec 16, Part 1. Introduction  Powder method A monochromatic X-ray beam scatters off the randomly oriented powder.
Determination of Protein Structure. Methods for Determining Structures X-ray crystallography – uses an X-ray diffraction pattern and electron density.
XRD Line Broadening With effects on Selected Area Diffraction (SAD) Patterns in a TEM MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani.
Internal – External Order We described symmetry of crystal habit (32 point groups) We also looked at internal ordering of atoms in 3-D structure (230 space.
(0,0) RECIPROCAL LATTICE (0,1) (1,1) (2,1) (3,1) REAL LATTICE a b a* b*
Followed by a few examples of
Discussion on Strategies Introductory Notes - omega vs. phi scans - beam polarization - single sweep vs. multi sweep - xtal shape as re-orientation/re-centering.
Chem Single Crystals For single crystals, we see the individual reciprocal lattice points projected onto the detector and we can determine the values.
Structural Analysis Apurva Mehta. Physics of Diffraction X-ray Lens not very good Mathematically Intersection of Ewald sphere with Reciprocal Lattice.
Structure of thin films by electron diffraction János L. Lábár.
IPCMS-GEMME, BP 43, 23 rue du Loess, Strasbourg Cedex 2
SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples
Tuesday, May 15 - Thursday, May 17, 2007
Xray crystallography Lasse Mårtensson, IFM-Chemistry.
(X-Ray Crystallography) X-RAY DIFFRACTION. I. X-Ray Diffraction  Uses X-Rays to identify the arrangement of atoms, molecules, or ions within a crystalline.
John Bargar 2nd Annual SSRL School on Hard X-ray Scattering Techniques in Materials and Environmental Sciences May 15-17, 2007 What use is Reciprocal Space?
X-Ray Diffraction ME 215 Exp#1. X-Ray Diffraction X-rays is a form of electromagnetic radiation having a range of wavelength from nm (0.01x10 -9.
X-ray Diffraction Outline Crystals and Bragg Diffraction
X. Low energy electron diffraction (LEED)
Introduction to Macromolecular X-ray Crystallography Biochem 300 Borden Lacy Print and online resources: Introduction to Macromolecular X-ray Crystallography,
Peak intensities Peak widths
Stanford Synchrotron Radiation Laboratory More Thin Film X-ray Scattering: Polycrystalline Films Mike Toney, SSRL 1.Introduction (real space – reciprocal.
Applying X-Ray Diffraction in Material Analysis Dr. Ahmed El-Naggar.
PHYS 430/603 material Laszlo Takacs UMBC Department of Physics
Diffraction Basics Coherent scattering around atomic scattering centers occurs when x-rays interact with material In materials with a crystalline structure,
Last Time Brillouin Zones and Intro to Scattering
Peter J. LaPuma1 © 1998 BRUKER AXS, Inc. All Rights Reserved This is powder diffraction!
X-ray diffraction. Braggs' law = 2d hkl sin  hkl X-ray diffraction From this set of planes, only get reflection at one angle -  From this set of planes,
X-Ray Measurement Methods From Chapter 6 of Textbook 2 and other references Diffractometer Hull/Debye-Scherrer method Pinhole method Laue Method Rotating.
XRD allows Crystal Structure Determination What do we need to know in order to define the crystal structure? - The size of the unit cell and the lattice.
Assessing Single Crystal Diamond Quality
Physics 2170 – Spring Davisson – Germer experiment Homework set 7 is due Wednesday. Problem solving sessions.
Crystallography and Diffraction. Theory and Modern Methods of Analysis Lectures Electron Diffraction Dr. I. Abrahams Queen Mary University of London.
Interaction of X-Rays with Materials
Page 1 X-ray crystallography: "molecular photography" Object Irradiate Scattering lens Combination Image Need wavelengths smaller than or on the order.
X-ray powder diffractometer X-ray powder diffractometer.
Least squares & Rietveld Have n points in powder pattern w/ observed intensity values Y i obs Minimize this function: Have n points in powder pattern w/
X-ray diffraction X-rays discovered in 1895 – 1 week later first image of hand. X-rays have ~ 0.1 – few A No lenses yet developed for x-rays – so no possibility.
Page 1 Phys Baski Diffraction Techniques Topic #7: Diffraction Techniques Introductory Material –Wave-like nature of electrons, diffraction/interference.
The Muppet’s Guide to: The Structure and Dynamics of Solids XRD.
X-Ray Diffraction Spring 2011.
Today’s Lecture Interference Diffraction Gratings Electron Diffraction
Fourier transform from r to k: Ã(k) =  A(r) e  i k r d 3 r Inverse FT from k to r: A(k) = (2  )  3  Ã(k) e +i k r d 3 k X-rays scatter off the charge.
Crystallography : How do you do? From Diffraction to structure…. Normally one would use a microscope to view very small objects. If we use a light microscope.
Crystal Structure and Crystallography of Materials Chapter 14: Diffraction Lecture No. 2.
Lecture 53: X-ray crystallography. Electrons deflect x-rays We try to recreate electron density from the x-ray diffraction pattern Each point in space.
Presentation Outline ANAELU: 2-D XRD texture analysis Experimental 2D XRD patterns Representation of structure Simulation of single-crystal XRD Polycrystal.
SHKim 2007 Lecture 4 Reciprocal lattice “Ewald sphere” Sphere of reflection (diffraction) Sphere of resolution.
1 Least squares & Rietveld Have n points in powder pattern w/ observed intensity values Y i obs Minimize this function:
BL04 MSPD Materials Science and Powder Diffraction Aleksandr Missiul
1. Detector 2. Crystal diffraction conditions
CHARACTERIZATION OF THE STRUCTURE OF SOLIDS
The theory of diffraction
de Broglie Waves de Broglie argued
X-ray diffraction.
X-ray powder diffractometer.
Institut Laue-Langevin
What use is Reciprocal Space? An Introduction
Presentation transcript:

Recent Advances in Protein Powder Diffraction R.B. Von Dreele, XSD/IPNS Argonne National Laboratory, USA “Reaching for High Resolution in Protein Powder Diffraction” Thanks – Peter Stephens, Peter Lee, US DOE/OS/BES

2 What is a powder? - polycrystalline mass All orientations of crystallites possible Sample: 1  l powder of 1  m crystallites - ~10 9 particles Single crystal reciprocal lattice - smeared into spherical shells - the overlap problem – lost information Packing efficiency – typically 50% Spaces – air, solvent, etc.

3 d* 1/ Powder diffraction - reciprocal space soso s Ewald sphere 22 Bragg’s Law Spherical reflection shells Smear in 3D Typical 1-D scan

4 Problem – Severe radiation damage of proteins Much worse at APS!! Happens in 10-20min!! , deg Powder patterns: Lysozyme – Multiple 1.15Å, RT, ~3hr ea.; ~10mg HEWL Radiation damage – initial X3b1 Xtal/analyzer detector 1 day

5 Faster data collection Beam focused to IP surface & IP offset 6-10cm up Sample (spun, 1x1mm, <1mg) Beam stop ~700mm ~0.6Å ~350mm Image Plate Detector – MAR345 “Guinier geometry”

6 11BMB – 10min scan1BM/MAR345 – 1sec exposure Compare image plate with analyzer/detector

7 Rings – protein pattern (HEWL) – X-rays 20kV on MAR345; <1mg HEWL Inner most ring – d~55Å (110) Reflection, lowest order for tetragonal lysozyme 2  ~ 0.67deg Beam stop holder Texture free sample & no graininess – 1  m “perfect” powder Resolution limit – 1.85Å Residual solvent scattering – background (Air, solvent & Kapton background subtracted) ~9000 F hkl for HEWL >2Å

8 Powder diffraction from 2D image plates (MAR345) Best focusing – best resolution FIT2D cake integration to d min = 2Å “resolution” ~0.035 o FWHM 300  m beam/pt. spread fxn. ~4X sample contribution!

9 HEWL comparison – 30s on 1BM Mar345 vs 10min on 11BM 20keV 30keV

10 Background problem – subtract air, liquid & Kapton Before subtraction: Gave too small R wp (<0.5%) from high background No sensitivity to structure After background subtraction: Weights: Compensate for 2D detector integration effect

11 Radiation damage – reflection intensities & positions APS 1BM - 30s exposures + 150s delay, 300K Full sequence wrt NaCl & pH – effects?? Immediate changes seen 2 stages? - 10min exposure Focus here: a up & c down

12 Multiple patterns – different lattice strains Buffer effect: Actually solvent effect? phthalate (<pH5) Phosphate(>pH5) Focus here Shortest exposure

13 Solvent & radiation damage induced lattice strains for HEWL Salt & pH effects Radiation exposure ~8% loss in 4.5m cf. FWHM o 2  ~ 0.02% o 2  Compare:  [M] = 0.07M;  pH = 0.07 (  [H+]~-15%) in 4.5m

14 Analysis: Induced lattice strain model – obey Laue symmetry From d-spacing expression partial derivatves wrt g ij of Bragg’s law gives And symmetrized for tetragonal a-axis strain for tetragonal is (c-axis similar) Peak shape function #5 in GSAS

Å resolution range – NaCl sequence 0.25M 1.25M Peak shifts! Obsd & calcd powder patterns Also for rad. dam. – just less

16 Profile fit – 1/5 patterns; R wp =1.84% 4x 20x

17 HEWL – superposition of 3 determinations (NaCl,pH5;NaCl,pH4 & RD) & H 2 O independently detn. H 2 O – many common positions (& some not) Variations? RMSD~0.4Å (all protein atoms)

18 Structure quality? Ramachandran plot – 90% most favored Total OMIT map – protein & H 2 O

19 HEWL I pH4 HEWL II pH5 HEWL III Rad dam HEWL I all/backbone, Å Vary NaCl, pH / /0.34 HEWL II all/backbone, Å Vary NaCl, pH5 0.44/ /0.40 HEWL III all/backbone, Å 1.25M NaCl, pH4, rad dam 0.42/ / LYT all/backbone, Å Best RT SC structure 1.35/ / / L all/backbone, Å Starting model 1.25/ / /0.77 HEWL results – structure comparisons Appropriate for 2Å resolution?

20 Compare – single pattern result (1JA2) & best single xtal 1JA2 - powder PDB 5 NaCl patterns - this work Rad. Dam. Seq. similar Q=57.63% Q=98.33% ERRAT2 – atom neighbor analysis - packing Compare: best HEWL single crystal result (low temp; xtal from shuttle!) Q=94.22% Howzat? PDB 1IEE

21 Overlap factor – effect of lattice strain better “effective” resolution? Overlap factor, R ij =1-  ij /2FWHM =1 if complete overlap, =0 if no overlap F i =  min(R ij ) for multipatterns 2 patterns 5 patterns  ~0  >2FWHM SC = 0 1 pattern

22 Sample size limit? in situ? 1 st experiments – NSLS X3b1; 1 analyzer/detector – 10mg HEWL slurry; 6hr scan Image plate – APS 1BM; MAR345; ~1mg HEWL slurry; 30s exposure CCD – APS 8BM (now defunct); ~15  g HEWL slurry; 10s exposure 2 of 1536 well plate – xtal growth test – not particularly optimized – corners <3Å

23 High throughput screening for crystallization – X-ray 8BM ~12keV 1536 well plate 1 st “real” expt. 4 plates & look for spots/rings? Compare optical pix ADSC 315 – 20Mb each pix = 5-6 DVDs/plate! ROBOT!! Craig Ogata, et al. & Blessing, et al.

24 Detector development – spatial resolution MAR345 – 300  m ADSC – 100  m 35  m – ideal match with sample

25 Tileable area detectors? Cover “best” part of powder pattern Tilted array – avoid “blind” spots in powder pattern Cover curved area to match resolution? Not necessarily spherical!

26 Conclusion – data combinations in proteins (at least HEWL) Protein powder diffraction  Image plates – lower powder resolution, but Better intensity measurement to higher diffr. resolution Induced lattice strain from RD, pH, salt, etc. variation  multiple powder patterns  lattice variation Recover powder resolution Result – higher powder & diffraction resolution  “better” protein structure (including water molecules) Future – smaller samples; better resolution Structure solution – multiple data set extraction of F o