Structure of a Membrane Proteins in Situ F. Jamilidinan, P. Schwander,D. K. Saldin.

Slides:



Advertisements
Similar presentations
Protein x-ray crystallography
Advertisements

Wave-Particle Duality Light quanta revisited and introduction to matter waves.
Introduction to protein x-ray crystallography. Electromagnetic waves E- electromagnetic field strength A- amplitude  - angular velocity - frequency.
Functions of Aquaporins in mammals. Kidney Cortex Nephron proximal tubules collecting duct Aqp0 urine concentration reabsorption of water into blood The.
Determination of Protein Structure. Methods for Determining Structures X-ray crystallography – uses an X-ray diffraction pattern and electron density.
By: Rachel Smith, Lauren Pyfer, Peter Xu IONIC RADIUS.
X-Ray Crystallography
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.
1 Ultrafast Electron Diffraction from Molecules in the Gas Phase Martin Centurion University of Nebraska – Lincoln.
Solid State Physics 2. X-ray Diffraction 4/15/2017.
CHE (Structural Inorganic Chemistry) X-ray Diffraction & Crystallography lecture 3 Dr Rob Jackson LJ1.16,
Computing Protein Structures from Electron Density Maps: The Missing Loop Problem I. Lotan, H. van den Bedem, A. Beacon and J.C. Latombe.
Lecture 3 – 4. October 2010 Molecular force field 1.
Hanging Drop Sitting Drop Microdialysis Crystallization Screening.
Methods: Cryo-Electron Microscopy Biochemistry 4000 Dr. Ute Kothe.
Mark J. van der Woerd1, Donald Estep2, Simon Tavener2, F
Angle- and internuclear separation- resolved strong field processes in molecules Grad student: Li Fang Funding : NSF-AMO May 26, 2010 DAMOP Houston, TX.
PHY 102: Waves & Quanta Topic 8 Diffraction II John Cockburn Room E15)
Gratings. Double Slit Resolution  The bright bands from a double slit are wide. Exact maximum difficult to determine  There is a broad area with some.
1 Bi 1 Lecture 3 Thursday, March 30, 2006 What is a Receptor? Receptors and Ion Channels as Examples of Proteins.
 In these set of slides we will try to visualize how constructive and destructive interference take place (using the Bragg’s view of diffraction as ‘reflection’
1 The Diffraction Phenomena in Atoms and Molecules.
Protein Structure Determination Part 2 -- X-ray Crystallography.
KHS ChemistryUnit 3.4 Structural Analysis1 Structural Analysis 3 Adv Higher Unit 3 Topic 4 Gordon Watson Chemistry Department, Kelso High School.
Lesson 5 Conditioning the x-ray beam
Introduction to Macromolecular X-ray Crystallography Biochem 300 Borden Lacy Print and online resources: Introduction to Macromolecular X-ray Crystallography,
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Chem X-ray Crystallography X-ray crystallography is an experimental technique that exploits the fact that X-rays are diffracted by the periodic.
 Four levels of protein structure  Linear  Sub-Structure  3D Structure  Complex Structure.
X-Ray Crystallography Susan Ahrens February 3, 2004.
Photogrammetry for Large Structures M. Kesteven CASS, CSIRO From Antikythera to the SKA Kerastari Workshop, June

Single-crystal X-ray Crystallography ● The most common experimental means of obtaining a detailed picture of a large molecule like a protein. ● Allows.
Structure to Elucidate Mechanism
EEW508 Structure of Surfaces Surface structure Rice terrace.
EAS Reconstruction with Cerenkov Photons Shower Simulation Reconstruction Algorithm Toy MC Study Two Detector Configuration Summary M.Z. Wang and C.C.
Coherent X-ray Diffraction (CXD) X-ray imaging of non periodic objects Campi G., De Caro L., Giannini C., Guagliardi A., Margonelli A., Pifferi A.
X RAY CRYSTALLOGRAPHY. WHY X-RAY? IN ORDER TO BE OBSERVED THE DIMENTIONS OF AN OBJECT MUST BE HALF OF THE LIGHT WAVELENGHT USED TO OBSERVE IT.
O. Gorobtsov 1,2, U. Lorenz 3, N. Kabachnik 4,5, I. A. Vartanyants 1,6 Electronic damage for short high-power x-ray pulses: its effect on single-particle.
Coherent X-ray Diffraction (CXD) X-ray imaging of non periodic objects Campi G., De Caro L., Giannini C., Guagliardi A., Margonelli A., Pifferi A.
Resolution Limits for Single-Slits and Circular Apertures  Single source  Two sources.
《Modern Research Methods in Polymer Science》
Announcements Grades (for Mid-term) in Web portal
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.
Epigenetic Processes from a Molecular Perspective INBRE Meeting 2/16/10.
Pattersons The “third space” of crystallography. The “phase problem”
Polymers (see Roe: Methods of X-ray and Neutron Scattering in Polymer Science (2000)) Polymers (see Roe: Methods of X-ray and Neutron Scattering in Polymer.
Atomic structure model
Coherent X-ray Diffraction (CXD) X-ray imaging of non periodic objects.
Physics 1202: Lecture 28 Today’s Agenda Announcements: –Midterm 2: solutions HW 8 this FridayHW 8 this Friday Diffraction –Review Polarization –Reflection.
Membrane protein session Erice Introduction Werner Kühlbrandt5 min Aquaporin 0Tom Walz30+5 min Na + /H + antiporterCarola Hunte30+5 min EM and.
X-Ray Diffraction Spring 2011.
--Experimental determinations of radial distribution functions --Potential of Mean Force 1.
Dynamically Polarized Solid Target for Neutron Scattering at the SNS PST 07 J.K. Zhao Neutron Scattering Sciences Division, Spallation Neutron Source Oak.
BioXFEL Journal Club Journal Club Presenter: George Calvey Pollack Group Cornell University.
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.
What is the interaction between x-rays and electrons Since x-rays are electromagnetic radiation they interact with atoms like any other radiation. Transmission—pass.
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.
X-RAY METHODS FOR ORIENTING CRYSTALS
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.
Page 1 Phase Determination by Creative BiostructureCreative Biostructure.
Compressive Coded Aperture Video Reconstruction
Organic Chemistry Lesson 21 X-ray crystallography.
Matter Waves Louis de Broglie
Introduction to Isomorphous Replacement and Anomalous Scattering Methods Measure native intensities Prepare isomorphous heavy atom derivatives Measure.
X Ray Diffraction © D Hoult 2009.
Matter Waves Louis de Broglie
Polarization via Rayleigh Scattering
Chapter 16: Electron Diffraction
Presentation transcript:

Structure of a Membrane Proteins in Situ F. Jamilidinan, P. Schwander,D. K. Saldin

TechniqueImportance RESEARCH Future SCENE

Why our work is important and what is our goal?  The targets of most medicinal drugs are membrane proteins  They are very difficult to crystallize  x-ray crystallography – trillions of molecules in identical orientations – not possible with most membrane proteins.  Can we work with partial alignment?  Ion channel proteins tend to be positioned within an membrane with random angles perpendicular to the membrane  However, their angular correlations are independent of particle orientation  Can we exploit this fact for structure determination?  The targets of most medicinal drugs are membrane proteins  They are very difficult to crystallize  x-ray crystallography – trillions of molecules in identical orientations – not possible with most membrane proteins.  Can we work with partial alignment?  Ion channel proteins tend to be positioned within an membrane with random angles perpendicular to the membrane  However, their angular correlations are independent of particle orientation  Can we exploit this fact for structure determination? 1 Solvent annulus Bilayer Incident x-rays Membrane Protein OUR TECHNIQUE  A collection of randomly oriented molecules give rise to a DP that looks angularly featureless.  However, the correlated scattering from each particle is the same.  The correlated signal tends to be drowned in the much larger uncorrelated signal from different molecules.  Assuming we can separate the signals, we exploit an algorithm for reconstructing a DP from its angular correlations.  Having reconstructed a single particle DP can get the projected potential by an iterative phasing algorithm  A collection of randomly oriented molecules give rise to a DP that looks angularly featureless.  However, the correlated scattering from each particle is the same.  The correlated signal tends to be drowned in the much larger uncorrelated signal from different molecules.  Assuming we can separate the signals, we exploit an algorithm for reconstructing a DP from its angular correlations.  Having reconstructed a single particle DP can get the projected potential by an iterative phasing algorithm 2 Why our work is important and what is our goal?  The targets of medicinal drugs are membrane proteins  Very difficult to crystallize => x-ray crystallography  The ion channel proteins tend to be positioned with random angles about this axis  We suggest a novel technique of determining the structures of membrane proteins in such configurations  The targets of medicinal drugs are membrane proteins  Very difficult to crystallize => x-ray crystallography  The ion channel proteins tend to be positioned with random angles about this axis  We suggest a novel technique of determining the structures of membrane proteins in such configurations 1 OUR TECHNIQUE 1.Generating simulated diffraction patterns from 10 randomly positioned and oriented model K- channel protein 2.recovery of a single-particle diffraction pattern from many particles diffraction patterns 3.Recovery of the projected electron density of a single particle 1.Generating simulated diffraction patterns from 10 randomly positioned and oriented model K- channel protein 2.recovery of a single-particle diffraction pattern from many particles diffraction patterns 3.Recovery of the projected electron density of a single particle 2 Future  Can overcome bottleneck for determining atomic scale structures of membrane proteins.  Will lead to a greater understanding of the action of medicinal drugs and perhaps other phenomena that depend on membrane proteins, such as photosynthesis  Can overcome bottleneck for determining atomic scale structures of membrane proteins.  Will lead to a greater understanding of the action of medicinal drugs and perhaps other phenomena that depend on membrane proteins, such as photosynthesis 3