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Methods: X-ray Crystallography. Biochemistry 4000 Dr. Ute Kothe. Why X-rays?. Optics: Limit of resolution ~ l /2 Distance between atoms: 0.1 – 0.3 nm Wavelenght of X-rays: 0.1 – 10 nm Allows structure determination at atomic resolution Problem: No lenses available for X-rays

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Methods x ray crystallography

Methods:X-ray Crystallography

Biochemistry 4000

Dr. Ute Kothe


Why x rays
Why X-rays?

  • Optics:

  • Limit of resolution ~ l/2

  • Distance between atoms: 0.1 – 0.3 nm

  • Wavelenght of X-rays: 0.1 – 10 nm

  • Allows structure determination

    at atomic resolution

    Problem:

    No lenses available for X-rays

    (as for visible light in microscope)

    Remember:

    Wavelength, Amplitude, Phase


Overview of steps
Overview of steps

Growing a Crystal

Collecting X-ray diffraction pattern

Solving of Phase Problem

Calculate Electron Density Map

Constructing a Structural Model

Refining the Structural Model


Growth of crystals background
Growth of Crystals - Background

Why? Diffraction pattern of single molecule too weak for detection

=> sum of several diffraction patterns of identically oriented

molecules with identical conformation

Porcine Elastase

Supersaturated Solution: Concentration higher than intrinsic solubility S0


Growth of crystals approaches
Growth of Crystals - Approaches

Hanging Drop Method:

  • Empirical Approach:

  • Test hundreds of conditions

  • Parameters:

  • pH

  • salt type & concentration

  • precipitant

  • (ammonium sulfate, polyethylene glycol, 2-methyl-2,4-dimethyl-pentane diol (MPD), propanol)

  • temperature (2 – 30°C)

  • protein concentration

  • (1 – 100 mg/ml)

  • additional substances

  • (substrates, inhibitors, cofactors etc.)

Alternative: Sitting Drop

Microdialysis


Description of crystals

a

γ

b

Description of Crystals

Unit cell:

characterized by edge length and angles

can contain several molecules

is repeated multiple times along the axis of the crystal

Assymetric Unit: minimal part of the unit cell which is related to other parts by defined symmetry operations


Space groups
Space Groups

  • Crystal can be described

  • by shape of unit cells (called lattice type, see figure) and symmetry type of asymmetric unit

  • 65 different space groups possible for natural biomolecules

    Example:

    P212121


Diffraction and interference
Diffraction and Interference

Huygen’s principle of diffraction:

Each point in front of a wavefront acts as a point of progapation for a new wavelet.

b) Constructive interference of scattered waves

=> Amplitude = 2E

c) Destructive interference of scattered waves

=> Amplitude = 0 (wave 180° out of phase)


Bragg s law
Bragg’s Law

  • Requirement for

  • constructive interference:

  • 2 d sin θ = n l

  • n: integer values (0, 1, 2, ...)

  • If angle θ and wavelenght l are known, the distance d between planes can be determined.

Simplification: reflection at planes (one dimension: distance d of planes)!


Diffraction in 3d miller indices
Diffraction in 3D: Miller Indices

Van Laue Conditions replace Bragg’s Law

(too much to explain in Bchm 4000)

Instead of “n”, three Miller Indices (h, k, l) define the integer number of wavelenght that result in an observed reflection froma 3D crystal.

Example: 2 points in space

1D reflection

2D reflection


More diffraction patterns
More Diffraction Patterns

2D example:

Each diffraction spot corresponds to one set of Miller indices (h, k, l).

Friedel’s law:

I(h,k,l) = I(-h,-k,-l)

http://www.esc.cam.ac.uk/teaching/teaching.html


Diffraction photograph
Diffraction Photograph

  • Each spot contains information from all atoms!

  • “Pattern of spots” (diffraction pattern) allows determination of crystal parameters (size of unit cell, symmetry within unit cell).

  • Structural information has to de derived (see below) from difference in spot intensities.

  • To obtain enough information, diffraction photographs are taken at various different angles of the crystal in the X-ray beam.

X-ray diffraction photograph

of Sperm Whale Myoglobin crystal


The structure factor f s
The Structure Factor: F(S)

  • How to get to an electron density map from the intensities of reflections?

  • Intrinsic amplitude of scattered X-ray from each type of atom depends on its electron density r(xyz) (described by atomic scattering factor f)

  • f is used to describe scattering vector for each atom for one reflection (with Miller indices h,k,l)

  • Sum of atomic scattering vectors is molecular scattering factor F, also called structure factor (can be calculated for a given structure):

    • F(hkl) = ∫r(xyz) e-2pi(hx+ky+lz) Fourier Transformation


The phase problem
The Phase Problem

  • Continued: How to get to an electron density map from the intensities of reflections?

    • Fourier Transformation (other way around)

    • r(xyz) = ∫F(hkl) e2pi(hx+ky+lz)

    • Magnitude of F is proportional to square root of intensity:

    • |F(hkl)| ~ √ I(hkl)

    • Thus: r(xyz) = 1/NV ∑ ∑ ∑ √I(hkl) e-i(hkl) e2pi(hx+ky+lz)

    • h k l

Electron Density

Intensity

Phase

Missing Information to get electron density!


Molecular replacement
Molecular Replacement

  • Method to obtain Phase information

  • Only possible if structure of a very similar molecule is known (native vs. Mutant, close homolog), at least 25% sequence identity

  • Calculate structure factors Fcalc for known molecule

  • Compare with data set to estimate phase for known structure (acalc)

  • Use this Phase information together with observed structure factors (Fobs) to calculate first electron density map

  • Refine Structure (see below)


Multiple isomorphous replacement
Multiple Isomorphous Replacement

  • 2. Method to obtain Phase information

  • Use crystals containing heavy atoms at specific positions (isomorphous crystals) as well as crystal of native protein

  • Heavy atoms strongly diffract

  • Difference data set of heavy atom derivative and native crystals gives structure factors of heavy atoms only = limited data set

  • Can be used to determine position and phase of heavy atoms (as for small molecule crystals, Patterson function)

  • Needs to be done for at least 2 heavy atom derivatives to obtain enough information to estimate phase of native data set and to solve the structure


Multiple anomalous dispersion
Multiple Anomalous Dispersion

  • 3. Method to obtain Phase information

  • Use onecrystal containing heavy atoms at specific positions as well as crystal of native protein

  • Heavy atoms not only diffract X-rays, but also absorbs X-rays of certain wavelength

  • Using synchroton X-ray source, diffraction data are generated at different wavelenghts of the heavy-atom crystal

  • Different data sets can be used to obtain phase information similar to multiple isomorphous replacement


Electron density map
Electron Density Map

  • Computed electron density map can be represented by “chicken wire” on computer.

  • Knowing the primary sequence of a protein (or nucleic acid) the atoms can be placed by hand into the electron density map.

  • Rough, inaccurate model of protein structure

What about hydrogen atoms?


Structural refinement
Structural Refinement

  • Iterative Process:

  • model is subtly changed

  • Structure Factors are calculated (Fcalc) and compared by Rcrys factor with measured Fobs to see how well a model fits the data:

  • differences are minimized (minimal R)

  • good structure: Rcrys < 20% (0.2)

  • Problem:

  • R factor can be artifically lowered by adding more solvent

  • better Rfree: as Rcrys, but calculated with 10% reflections which have not been used for refinement (unbiased data set)


Resolution
Resolution

  • Limited by:

  • Quality of crystal (Conformational inhomogenities, Mobility of individual atoms)

  • Number of unique reflections used for structure determination (at least four times more than atoms required)

  • Typically not by wavelength

5Å - a helices roughly visible

3Å - peptide chain visible, side chains if sequence known

2Å - conformations of side chains visible


Temperature factor b factor
Temperature Factor (B factor)

  • Describes local imprecision in electron density

  • Calculated during structure refinement

  • Measured in Ų

  • The higher the B factor, the more imprecise the atom position.

  • Good protein structure: B < 20 - 30 Ų

  • Reasons for higher B factor:

  • Thermal motion of atom

  • Different conformations of side chain, i.e. lower occupancy at specific position

  • Protein disordered, e.g. In surface exposed loops


Other important parameters
Other Important Parameters

  • Protein backbone should have only allowed conformations (as described in Ramachandran plot)

  • Completenes of structure (should be >90%)


Parameters in publication
Parameters in Publication

Rasmussen et al., Science 2007


Protein data base
Protein Data Base

  • structure data (x, y, z coordinates of each atom) are submitted to Protein Data Base

  • freely accessible, structure can be downloaded and visualized with free programs such as RasMol or Swiss PDB Viewer


Native conformation
Native Conformation?

  • Is protein structure determined from crystal the same as

  • in vivo solution structure?

  • Most likely:

  • Crystals contain 40 – 60 % solvent, i.e. the protein is in simialr environment as in cell

  • Often proteins crystallize in different space groups with different crystal contacts between proteins, but the determined structure is the same, i.e. It is independent of crystal packing.

  • Often X-ray structures and solution NMR structures superimpose well.

  • Many enzymes are active in crystalline state

  • BUT: You never know! Exceptions are possible!


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