Nobel Laureates of X Ray Crystallography

Slides:



Advertisements
Similar presentations
Intensities Learning Outcomes By the end of this section you should: understand the factors that contribute to diffraction know and be able to use the.
Advertisements

Phasing Goal is to calculate phases using isomorphous and anomalous differences from PCMBS and GdCl3 derivatives --MIRAS. How many phasing triangles will.
Protein Structure and Physics. What I will talk about today… -Outline protein synthesis and explain the basic steps involved. -Go over the Chemistry of.
Protein x-ray crystallography
Introduction to protein x-ray crystallography. Electromagnetic waves E- electromagnetic field strength A- amplitude  - angular velocity - frequency.
Methods: X-ray Crystallography
Determination of Protein Structure. Methods for Determining Structures X-ray crystallography – uses an X-ray diffraction pattern and electron density.
Nobel Laureates contributing to X-ray, diffraction and crystallography InsulinInsulin crystals.
X-Ray Crystallography
EEE539 Solid State Electronics
Computing Protein Structures from Electron Density Maps: The Missing Loop Problem I. Lotan, H. van den Bedem, A. Beacon and J.C. Latombe.
Hanging Drop Sitting Drop Microdialysis Crystallization Screening.
Experimental Phasing Andrew Howard ACA Summer School 22 July 2005.
Energetics and kinetics of protein folding. Comparison to other self-assembling systems?
Proteins are made by linking amino acids Protein Structure Review and Refinement Introduction Brian Bahnson Dept of Chemistry & Biochemistry, University.
Mid-term.
Overview of the Phase Problem
Computing and Chemistry 3-41 Athabasca Hall Sept. 16, 2013.
Protein Structure Determination Part 2 -- X-ray Crystallography.
Chapter 12 Protein Structure Basics. 20 naturally occurring amino acids Free amino group (-NH2) Free carboxyl group (-COOH) Both groups linked to a central.
X-ray and NMR Topic 7 Chapter 4 & 5, Du and Bourne “Structural Bioinformatics”
MOLECULAR REPLACEMENT Basic approach Thoughtful approach Many many thanks to Airlie McCoy.
Bragg Planes How to do a Fourier transform on paper with no calculations at all.
Patterson Space and Heavy Atom Isomorphous Replacement
 Four levels of protein structure  Linear  Sub-Structure  3D Structure  Complex Structure.
The ‘phase problem’ in X-ray crystallography What is ‘the problem’? How can we overcome ‘the problem’?
Single-crystal X-ray Crystallography ● The most common experimental means of obtaining a detailed picture of a large molecule like a protein. ● Allows.
Chem Structure Factors Until now, we have only typically considered reflections arising from planes in a hypothetical lattice containing one atom.
Phasing Today’s goal is to calculate phases (  p ) for proteinase K using PCMBS and EuCl 3 (MIRAS method). What experimental data do we need? 1) from.
1. Diffraction intensity 2. Patterson map Lecture
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.
Methods in Chemistry III – Part 1 Modul M.Che.1101 WS 2010/11 – 8 Modern Methods of Inorganic Chemistry Mi 10:15-12:00, Hörsaal II George Sheldrick
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.
What is the problem? How was the problem solved?
Protein Structure Determination Lecture 4 -- Bragg’s Law and the Fourier Transform.
Pattersons The “third space” of crystallography. The “phase problem”
Atomic structure model
X-ray crystallography – an overview (based on Bernie Brown’s talk, Dept. of Chemistry, WFU) Protein is crystallized (sometimes low-gravity atmosphere is.
Before Beginning – Must copy over the p4p file – Enter../xl.p4p. – Enter../xl.hkl. – Do ls to see the files are there – Since the.p4p file has been created.
X-Ray Diffraction Spring 2011.
Methods in Chemistry III – Part 1 Modul M.Che.1101 WS 2010/11 – 9 Modern Methods of Inorganic Chemistry Mi 10:15-12:00, Hörsaal II George Sheldrick
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.
Lecture 10 CS566 Fall Structural Bioinformatics Motivation Concepts Structure Solving Structure Comparison Structure Prediction Modeling Structural.
Today: compute the experimental electron density map of proteinase K Fourier synthesis  (xyz)=  |F hkl | cos2  (hx+ky+lz -  hkl ) hkl.
Lecture 3 Patterson functions. Patterson functions The Patterson function is the auto-correlation function of the electron density ρ(x) of the structure.
Crystal Structure and Crystallography of Materials Chapter 13: Diffraction Lecture No. 1.
Match diffraction patterns to electron densities Electron densities (one unit cell) Diffraction patterns.
Cont. Proteomics Structural Genomics Describes the experimental and analytical techniques that are used to determine the structure of proteins and RNA.
Page 1 Phase Determination by Creative BiostructureCreative Biostructure.
Atomic Mass,Formula mass and Molecular mass
Polarization Dependence in X-ray Spectroscopy and Scattering
Stony Brook Integrative Structural Biology Organization
Computational Structure Prediction
Crystallography of Biological Macromolecules History
Seminar on X-ray Diffraction
Organic Chemistry Lesson 21 X-ray crystallography.
Chap 3 Scattering and structures
The theory of diffraction
Complete automation in CCP4 What do we need and how to achieve it?
Dihedral angle preferences of DNA and RNA binding
Phasing Today’s goal is to calculate phases (ap) for proteinase K using MIRAS method (PCMBS and GdCl3). What experimental data do we need? 1) from native.
Protein Structure Determination
Introduction to Isomorphous Replacement and Anomalous Scattering Methods Measure native intensities Prepare isomorphous heavy atom derivatives Measure.
S. Takeda, A. Yamashita, K. Maeda, Y. Maeda
Diffraction T. Ishikawa Part 1 Kinematical Theory 1/11/2019 JASS02.
Determining protein structures
Volume 15, Issue 9, Pages (September 2007)
Introduction During the last years the use of Fourier Transform Infrared spectroscopy (FTIR) to determine the structure of biological macromolecules.
A. The Solid State Classification of Solid Structures
Inelastic Neutron Scattering Correction
Presentation transcript:

Nobel Laureates of X Ray Crystallography Max von Laue - 1914 Nobel Prize in Physics Bragg(s) - 1915 Nobel Prize in Physics. Dorothy Hodgkin – 1964 Nobel Prize in Chemistry Hauptman and Karle - 1985 Nobel Prize in Chemistry Roderick MacKinnon and Peter Agre – 2003 Nobel Prize in Chemistry

ψ φ Cα Cα

Levinthal's paradox How many backbone conformations of a 300 residue protein are possible? Only taking into account Phi and Psi angles, approximately 10³°° conformations How is the right conformation found in our lifetime? Answer: Only some angle combinations are energetically favorable, hence only a limited amount of structural conformations are possible

Steps To Solving The Structure Of A Protein

When X-rays strike a macromolecular crystal, the atoms in the molecules produce scattered X-ray waves which combine to give a complex diffraction pattern consisting of waves of different amplitudes

What is measured experimentally are the amplitudes and positions of the scattered X-ray waves from the crystal X-ray crystallography provides the positions of all non-hydrogen atoms The origin of each wave must be determined so that they sum to give an image instead of a “sea of noise” Phase values must be assigned to all of the recorded data; sometimes done computationally, but is usually done experimentally by labeling the protein with one or more heavy atoms whose position in the crystal can be determined independently

Electron Density Calculation Diffraction amplitudes = FT{Electron density} Take the inverse FT of the diffraction pattern to regenerate the electron density Shooting a crystal with X-rays and obtaining a diffraction pattern is the same as taking the Fourier transform of a compound. Hence, taking the Fourier transform again gives us the original structure.

After shooting Our Protein with X-rays And getting the FT Taking the FT of the FT RESTORES the original Data (mostly) Our Protein A very simple example of Fourier and Inverse Fourier transforms

The scattered x-rays have amplitudes given by Fourier coefficients of electron density Possible to measure amplitudes If we could also measure phases, we could compute electron density by inverse Fourier transform We then fit a model to the density Phases are extremely difficult to measure

Quick Recap Crystallize Protein (if humanly possible) Measuring diffraction amplitudes Using a computer to calculate electron density Building a model consistent w/ density

Quality Of a Structure R-factors represent the percentage disagreement between the observed diffraction pattern and that calculated from the final model R-factors of around 20% or less are considered well determined structures that are expected to contain relatively few errors

Express the resolution of a structure in terms of a distance

Molecular Replacement Use an analogous structure (similar amino acid sequence) and apply to the structure you are trying to determine “Replacement” actually means 'relocation, repositioning‘ atoms.

(Multiple) Isomorphous Replacement