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Physics 570 Michael Martynowycz

Physics 570 Michael Martynowycz - Illinois Institute of ...csrri.iit.edu/~segre/phys570/12S/presentations/martynowycz.pdf · Michael Martynowycz . The Structural Basis for Specificity

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  • Physics 570 Michael Martynowycz

  • The Structural Basis for Specificity in Human ABO(H) Blood Group Biosynthesis Patenaude et al.

    Two glycotransferases of differing sugar donors: GTA, GTB

    Differ by four residues Only one found to be critical Needed for H-antigen binding Structures resolve binding sites

  • Why X-Rays?

    Recall Braggs Law 2 =

    Average bond length ~1-2 X-Rays generally ~1

    Comparatively, visible light is ~5500 X-Rays are in a resolution sweet spot

    for biological samples

  • Protein Crystallography

    Purification Crystallization Mounting Data Collection Data Processing Structure Solution Structure Analysis

    Ref. 8

  • Pre-Work Protein extracted from E. coli

    Purified via affinity columns

    Crystallized at 18 via hanging drop diffusion Evaporates the sample to needed concentration

    Sample placed within an X-Ray chamber

    Controlled temperature and vacuum required

    Ref. 6

  • The X-Rays (Data Collection)

    Overwhelmingly elastic scattering

    Requires formation of ordered domains Symmetry groups describing a primitive unit

    cell, c222 in this case Ultimately resolve the electron density, (,, )

    Ref. 4

  • X-Ray Optics of Crystallography

    Recall that for X-Rays, = 1 +

    = 22

    = 2

    Optical phenomena

    arise from difference in path length, seen here as r

    Ref. 2

  • Crystal Reflection Path difference can

    be seen as: = =

    Geometry yields:

    = 2 sin The phase

    difference is then given by: = 2

    = 2

    = 2

    Ref. 2

  • Electron density If is scattered to , from the source at , then:

    = 2 is the electron

    density at that point This can be

    integrated over a finite volume to get the total amplitude and phase:

    = 2

    Which can be Fourier Transformed in order to obtain the total electron density:

    = 2

  • What is measured? We do not directly

    measure amplitude, we measure intensity

    2 Phase information is

    lost, and must be reconstructed later

    Reconstruction is possible due to periodicity of the lattice

    We may say the transformed amplitude(unit) is then:

    = 2

    If we translate each D by some a, then:

    () 2=0 = ()

  • Protein structures The method described

    does not work directly Heavy molecules

    attached to the larger in set locations

    Diffraction patters are taken with and without the heavy molecules and solved as a superposition

    Ref. 2

  • Current methodology The modern approach

    is to tune the X-Rays to the absorption edge of the heavy particles

    This results in a known phase and amplitude shift

    Essentially the same idea as isomorphous replacement, but much faster

    Ref. 2

  • The result Intensity gathered by

    a charge-coupled device(CCD) detector

    Initial data passed to HKL2000 (software) to prepare data

    Rendering done by ARP/wARP (software)

    Final rendering done by SETOR, and placed on the Protein Data Bank PDB.org

    Ref. 1

  • References Online sources

    [1]Nature Structural Biology, Vol 9, nu 9, sept 2002

    [2]Encyclopedia of Optical Engineering, Robert M. Sweet

    [3]Elements of modern X-Ray Physics 2nd ed, Wiley 2012, Als-Nielsen, McMorrow

    [4]http://en.wikipedia.org/wiki/X-ray_crystallography

    [5]http://web.pdx.edu/~pmoeck/phy381/Topic5a-XRD.pdf

    [6]http://www.bio.davidson.edu/courses/molbio/molstudents/spring2003/kogoy/protein.html

    [7]http://www.proteincrystallography.org/

    [8]http://www.pdb.org/pdb/home/home.do

    http://en.wikipedia.org/wiki/X-ray_crystallographyhttp://en.wikipedia.org/wiki/X-ray_crystallographyhttp://web.pdx.edu/~pmoeck/phy381/Topic5a-XRD.pdfhttp://web.pdx.edu/~pmoeck/phy381/Topic5a-XRD.pdfhttp://web.pdx.edu/~pmoeck/phy381/Topic5a-XRD.pdfhttp://www.bio.davidson.edu/courses/molbio/molstudents/spring2003/kogoy/protein.htmlhttp://www.bio.davidson.edu/courses/molbio/molstudents/spring2003/kogoy/protein.htmlhttp://www.bio.davidson.edu/courses/molbio/molstudents/spring2003/kogoy/protein.htmlhttp://www.bio.davidson.edu/courses/molbio/molstudents/spring2003/kogoy/protein.htmlhttp://www.proteincrystallography.org/http://www.proteincrystallography.org/http://www.pdb.org/pdb/home/home.dohttp://www.pdb.org/pdb/home/home.do

    Final PresentationThe Structural Basis for Specificity in Human ABO(H) Blood Group BiosynthesisPatenaude et al.Why X-Rays?Protein CrystallographyPre-WorkThe X-Rays (Data Collection)X-Ray Optics of CrystallographyCrystal ReflectionElectron densityWhat is measured?Protein structuresCurrent methodologyThe resultSlide Number 14