5E79 image
Entry Detail
PDB ID:
5E79
Keywords:
Title:
Macromolecular diffractive imaging using imperfect crystals
Biological Source:
PDB Version:
Deposition Date:
2015-10-12
Release Date:
2017-02-08
Method Details:
Experimental Method:
Resolution:
3.50 Å
R-Value Free:
0.33
R-Value Work:
0.32
R-Value Observed:
0.32
Space Group:
P 1
Macromolecular Entities
Polymer Type:polypeptide(L)
Description:Photosystem II protein D1 1
Chain IDs:A, T (auth: a)
Chain Length:334
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Photosystem II CP47 reaction center protein
Chain IDs:B, U (auth: b)
Chain Length:504
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Photosystem II CP43 reaction center protein
Chain IDs:C, V (auth: c)
Chain Length:451
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Photosystem II D2 protein
Chain IDs:D, W (auth: d)
Chain Length:342
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Cytochrome b559 subunit alpha
Chain IDs:E, X (auth: e)
Chain Length:81
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Cytochrome b559 subunit beta
Chain IDs:F, Y (auth: f)
Chain Length:34
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Photosystem II reaction center protein H
Chain IDs:G (auth: H), Z (auth: h)
Chain Length:65
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Photosystem II reaction center protein I
Chain IDs:H (auth: I), AA (auth: i)
Chain Length:38
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Photosystem II reaction center protein J
Chain IDs:I (auth: J), BA (auth: j)
Chain Length:38
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Photosystem II reaction center protein K
Chain IDs:J (auth: K), CA (auth: k)
Chain Length:37
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Photosystem II reaction center protein L
Chain IDs:K (auth: L), DA (auth: l)
Chain Length:37
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Photosystem II reaction center protein M
Chain IDs:L (auth: M), EA (auth: m)
Chain Length:34
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Photosystem II manganese-stabilizing polypeptide
Chain IDs:M (auth: O), FA (auth: o)
Chain Length:243
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Photosystem II reaction center protein T
Chain IDs:N (auth: T), GA (auth: t)
Chain Length:30
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Photosystem II 12 kDa extrinsic protein
Chain IDs:O (auth: U), HA (auth: u)
Chain Length:97
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Cytochrome c-550
Chain IDs:P (auth: V), IA (auth: v)
Chain Length:137
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Photosystem II reaction center X protein
Chain IDs:R (auth: X), KA (auth: x)
Chain Length:39
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Photosystem II reaction center protein Ycf12
Chain IDs:Q (auth: Y), JA (auth: y)
Chain Length:29
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Polymer Type:polypeptide(L)
Description:Photosystem II reaction center protein Z
Chain IDs:S (auth: Z), LA (auth: z)
Chain Length:62
Number of Molecules:2
Biological Source:Thermosynechococcus elongatus (strain BP-1)
Primary Citation

Abstact

The three-dimensional structures of macromolecules and their complexes are mainly elucidated by X-ray protein crystallography. A major limitation of this method is access to high-quality crystals, which is necessary to ensure X-ray diffraction extends to sufficiently large scattering angles and hence yields information of sufficiently high resolution with which to solve the crystal structure. The observation that crystals with reduced unit-cell volumes and tighter macromolecular packing often produce higher-resolution Bragg peaks suggests that crystallographic resolution for some macromolecules may be limited not by their heterogeneity, but by a deviation of strict positional ordering of the crystalline lattice. Such displacements of molecules from the ideal lattice give rise to a continuous diffraction pattern that is equal to the incoherent sum of diffraction from rigid individual molecular complexes aligned along several discrete crystallographic orientations and that, consequently, contains more information than Bragg peaks alone. Although such continuous diffraction patterns have long been observed--and are of interest as a source of information about the dynamics of proteins--they have not been used for structure determination. Here we show for crystals of the integral membrane protein complex photosystem II that lattice disorder increases the information content and the resolution of the diffraction pattern well beyond the 4.5-ångström limit of measurable Bragg peaks, which allows us to phase the pattern directly. Using the molecular envelope conventionally determined at 4.5 ångströms as a constraint, we obtain a static image of the photosystem II dimer at a resolution of 3.5 ångströms. This result shows that continuous diffraction can be used to overcome what have long been supposed to be the resolution limits of macromolecular crystallography, using a method that exploits commonly encountered imperfect crystals and enables model-free phasing.

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