Introduction to Isomorphous Replacement and Anomalous Scattering Methods Measure native intensities Prepare isomorphous heavy atom derivatives Measure.

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.
Does instruction lead to learning?. A mini-quiz – 5 minutes 1.Write down the ground state wavefunction of the hydrogen atom? 2.What is the radius of the.
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
Overview of the Phase Problem
Determination of Protein Structure. Methods for Determining Structures X-ray crystallography – uses an X-ray diffraction pattern and electron density.
M.I.R.(A.S.) S.M. Prince U.M.I.S.T.. The only generally applicable way of solving macromolecular crystal structure No reliance on homologous structure.
M.I.R.(A.S.) S.M. Prince U.M.I.S.T.. The only generally applicable way of solving macromolecular crystal structure No reliance on homologous structure.
X-Ray Crystallography
EEE539 Solid State Electronics
Solid State Physics 2. X-ray Diffraction 4/15/2017.
A Brief Description of the Crystallographic Experiment
Chemical order & disorder in metallic alloy Calculation of Bragg and Diffuse Scattering Correlation length in the Mean-Field approach Correlation Length.
Hanging Drop Sitting Drop Microdialysis Crystallization Screening.
3. Crystals What defines a crystal? Atoms, lattice points, symmetry, space groups Diffraction B-factors R-factors Resolution Refinement Modeling!
Copyright © Cengage Learning. All rights reserved. 10 Introduction to the Derivative.
Experimental Phasing Andrew Howard ACA Summer School 22 July 2005.
02-1 Physics I Class 02 One-Dimensional Motion Definitions.
X-ray diffraction Meet in the LGRT lab Again, will hand in worksheet, not a formal lab report Revision exercise – hand in by April 17 th class.
Fourier transform. Fourier transform Fourier transform.
Direct Methods By Fan Hai-fu, Institute of Physics, Beijing Direct Methods By Fan Hai-fu, Institute of Physics, Beijing
Overview of the Phase Problem
CHE (Structural Inorganic Chemistry) X-ray Diffraction & Crystallography lecture 2 Dr Rob Jackson LJ1.16,
MOLECULAR REPLACEMENT Basic approach Thoughtful approach Many many thanks to Airlie McCoy.
1 Refinement parameters What are the parameters to be determined? atom positional parameters atom thermal motion parameters atom site occupancy parameters.
Introduction to Patterson Function and its Applications
Patterson Space and Heavy Atom Isomorphous Replacement
In serial femtosecond crystallography (SFX) with hard X-ray free-electron laser as light source, a set of three-dimensional single-crystal diffraction.
The ‘phase problem’ in X-ray crystallography What is ‘the problem’? How can we overcome ‘the problem’?
Chem Patterson Methods In 1935, Patterson showed that the unknown phase information in the equation for electron density:  (xyz) = 1/V ∑ h ∑ k.
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
Electronic Band Structures electrons in solids: in a periodic potential due to the periodic arrays of atoms electronic band structure: electron states.
THE PHASE PROBLEM Electron Density
Linear and Planar Atomic Densities
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”
The Structure and Dynamics of Solids
Atomic structure model
Anomalous Differences Bijvoet differences (hkl) vs (-h-k-l) Dispersive Differences 1 (hkl) vs 2 (hkl) From merged (hkl)’s.
Electron Density Structure factor amplitude defined as: F unit cell (S) = ∫ r  (r) · exp (2  i r · S) dr Using the inverse Fourier Transform  (r) =
Review Of Statistical Mechanics Continued
X-ray Crystallography Kalyan Das. Electromagnetic Spectrum to 10 nM 400 to 700 nM to nM 10 to 400 nM 700 to 10 4 nM X-ray was discovered.
--Experimental determinations of radial distribution functions --Potential of Mean Force 1.
BioXFEL Journal Club Journal Club Presenter: George Calvey Pollack Group Cornell University.
Phasing in Macromolecular Crystallography
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.
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.
Hanyang University 1/18 Seminar on Microwave and Optical Communication Wonhong Jeong
Amyloid Precursor Protein (APP)
Stony Brook Integrative Structural Biology Organization
Procedure for structure analysis Overview of strategy
Continuity equation Physical meaning.
The theory of diffraction
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.
Notes: problem with illustrating gauss’ law and polarization divergence is that this is valid for continuous functions, and we cant illustrate that well.
Nobel Laureates of X Ray Crystallography
S. Takeda, A. Yamashita, K. Maeda, Y. Maeda
Diffraction T. Ishikawa Part 1 Kinematical Theory 1/11/2019 JASS02.
r(xyz)=S |Fhkl| cos2p(hx+ky+lz -ahkl)
Volume 93, Issue 7, Pages (June 1998)
Crystal Structures of a Novel Ferric Reductase from the Hyperthermophilic Archaeon Archaeoglobus fulgidus and Its Complex with NADP+  Hsiu-Ju Chiu, Eric.

Presentation transcript:

Introduction to Isomorphous Replacement and Anomalous Scattering Methods Measure native intensities Prepare isomorphous heavy atom derivatives Measure derivative intensities Scale native and derivative data Determine heavy atom positions and occupancies Correlate origin and hand between derivatives Compute protein phases

An isomorphous derivative crystal is one in which the only changes in electron density between it and the native crystal are peaks at the sites of heavy atom substitution. The above definition implies no appreciable changes in packing contacts or unit cell constants and no change in space group. Does it ever happen? No. Changes usually occur in protein conformation near the heavy atom binding sites, and solvent molecules are displaced. Fortunately, these effects are often small, localized and mostly alter the low resolution data. Nevertheless, for isomorphous crystals as we have defined them, the structure factor for any reflection in the derivative crystal can be expressed as the vector sum of the corresponding structure factors for the native and “heavy atom” crystals, where the “heavy atom” crystal is a hypothetical crystal with the same cell and symmetry as the native but containing only the heavy atoms. It is instructive to consider the consequences of this relationship from both an algebraic and geometric point of view.

PHASE DETERMINATION BY SINGLE ISOMORPHOUS REPLACEMENT.