N Khazanovich, KS Bateman, M Chernaia, M Michalak, MNG James  Structure 

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Crystal structure of the yeast cell-cycle control protein, p13suc1, in a strand-exchanged dimer  N Khazanovich, KS Bateman, M Chernaia, M Michalak, MNG James  Structure  Volume 4, Issue 3, Pages 299-309 (March 1996) DOI: 10.1016/S0969-2126(96)00034-2

Figure 1 The two forms of p13suc1. (a) The monomer of p13suc1, observed in the hexagonal space group (p13hex) [19]. (b) The strand-exchanged dimer of p13suc1 (p13or). Two symmetry-related CHAPS molecules are present in the arch of the dimer. Labelling of secondary structure of p13or corresponds to that shown in Figure 3. The first α-helix has been designated as two helical segments, α1′ and α1″, separated by a kink at Pro20. The first β-strand is also divided into β1′ and β1″ by a β-bulge at Pro29. Strand β4∗ originates from the strand-exchange partner. (Figure generated using MOLSCRIPT [37].) Structure 1996 4, 299-309DOI: (10.1016/S0969-2126(96)00034-2)

Figure 1 The two forms of p13suc1. (a) The monomer of p13suc1, observed in the hexagonal space group (p13hex) [19]. (b) The strand-exchanged dimer of p13suc1 (p13or). Two symmetry-related CHAPS molecules are present in the arch of the dimer. Labelling of secondary structure of p13or corresponds to that shown in Figure 3. The first α-helix has been designated as two helical segments, α1′ and α1″, separated by a kink at Pro20. The first β-strand is also divided into β1′ and β1″ by a β-bulge at Pro29. Strand β4∗ originates from the strand-exchange partner. (Figure generated using MOLSCRIPT [37].) Structure 1996 4, 299-309DOI: (10.1016/S0969-2126(96)00034-2)

Figure 2 Electron density of the strand-exchange region. (a) Electron density with phases derived from the molecular replacement model (p13hex), initially refined with X-PLOR [32]. The phasing model included a loop connecting β3 to β4, rather than an exchanged strand. Residues Tyr85–Pro92 of the final refined model are shown (2Fo–Fc density, contoured at 1σ). (b) Electron density with phases derived from the final refined model (p13or) omitting residues 85–92. A water molecule in this region (represented by +) was not omitted. The final refined model is shown, residues Tyr85–Pro92 (Fo–Fc density, contoured at 2σ). Structure 1996 4, 299-309DOI: (10.1016/S0969-2126(96)00034-2)

Figure 2 Electron density of the strand-exchange region. (a) Electron density with phases derived from the molecular replacement model (p13hex), initially refined with X-PLOR [32]. The phasing model included a loop connecting β3 to β4, rather than an exchanged strand. Residues Tyr85–Pro92 of the final refined model are shown (2Fo–Fc density, contoured at 1σ). (b) Electron density with phases derived from the final refined model (p13or) omitting residues 85–92. A water molecule in this region (represented by +) was not omitted. The final refined model is shown, residues Tyr85–Pro92 (Fo–Fc density, contoured at 2σ). Structure 1996 4, 299-309DOI: (10.1016/S0969-2126(96)00034-2)

Figure 3 Sequence alignment of p13suc1 from S. pombe and its homologues, CKS1 from S. cerevisiae, human CksHs1 and CksHs2, and CKS1 from Patella vulgata [16]. p13suc1 numbering and secondary structure elements of p13or are indicated above the sequence. (α1′ and α2 are 310-helices.) The residues involved in strand exchange in p13suc1 and in CksHs2 are shown bold. Boxes indicate conserved residues. Q16 in the S. cerevisiae CKS1 sequence indicates a run of 16 glutamine residues. Structure 1996 4, 299-309DOI: (10.1016/S0969-2126(96)00034-2)

Figure 4 The strand-exchange regions of p13or and CksHs2. (a) p13or, residues 83–93. (b) CksHs2, subunits C, residues 57–69. In both cases, primed numbers indicate residues of the symmetry-related strand. Structure 1996 4, 299-309DOI: (10.1016/S0969-2126(96)00034-2)

Figure 4 The strand-exchange regions of p13or and CksHs2. (a) p13or, residues 83–93. (b) CksHs2, subunits C, residues 57–69. In both cases, primed numbers indicate residues of the symmetry-related strand. Structure 1996 4, 299-309DOI: (10.1016/S0969-2126(96)00034-2)

Figure 5 The strand-exchanged dimers. (a) Superposition of the CksHs2 monomer (magenta) [21] on the p13or monomer (red). Also shown are strand-exchange partners of both molecules (CksHs2, cyan and p13or, yellow). Arrows indicate residues in the strand-exchange region, Tyr85 and Pro92, which have significantly different φ and ψ angles in p13or and in CksHs2. The loop between α2 and α3, which is longer in p13suc1 than in CksHs2, is also indicated. (b) Comparison of the p13suc1 dimers with the left-hand monomer superimposed illustrates a twist in the dimer. The p13or dimer is shown in red. The two dimers in the asymmetric unit of the P212121 structure [22] are shown in orange and magenta. (c) Superposition of the strand-exchange region of two p13suc1 dimers from the P212121 asymmetric unit (yellow and blue) with p13or (red). In p13or, two ordered water molecules, related by twofold symmetry, are present. Each dimer from the space group P212121 has only one water molecule in this region. (Panels (a) and (b) generated with the program Raster3D [38]; panel (c) generated with MOLSCRIPT [37].) Structure 1996 4, 299-309DOI: (10.1016/S0969-2126(96)00034-2)

Figure 5 The strand-exchanged dimers. (a) Superposition of the CksHs2 monomer (magenta) [21] on the p13or monomer (red). Also shown are strand-exchange partners of both molecules (CksHs2, cyan and p13or, yellow). Arrows indicate residues in the strand-exchange region, Tyr85 and Pro92, which have significantly different φ and ψ angles in p13or and in CksHs2. The loop between α2 and α3, which is longer in p13suc1 than in CksHs2, is also indicated. (b) Comparison of the p13suc1 dimers with the left-hand monomer superimposed illustrates a twist in the dimer. The p13or dimer is shown in red. The two dimers in the asymmetric unit of the P212121 structure [22] are shown in orange and magenta. (c) Superposition of the strand-exchange region of two p13suc1 dimers from the P212121 asymmetric unit (yellow and blue) with p13or (red). In p13or, two ordered water molecules, related by twofold symmetry, are present. Each dimer from the space group P212121 has only one water molecule in this region. (Panels (a) and (b) generated with the program Raster3D [38]; panel (c) generated with MOLSCRIPT [37].) Structure 1996 4, 299-309DOI: (10.1016/S0969-2126(96)00034-2)

Figure 5 The strand-exchanged dimers. (a) Superposition of the CksHs2 monomer (magenta) [21] on the p13or monomer (red). Also shown are strand-exchange partners of both molecules (CksHs2, cyan and p13or, yellow). Arrows indicate residues in the strand-exchange region, Tyr85 and Pro92, which have significantly different φ and ψ angles in p13or and in CksHs2. The loop between α2 and α3, which is longer in p13suc1 than in CksHs2, is also indicated. (b) Comparison of the p13suc1 dimers with the left-hand monomer superimposed illustrates a twist in the dimer. The p13or dimer is shown in red. The two dimers in the asymmetric unit of the P212121 structure [22] are shown in orange and magenta. (c) Superposition of the strand-exchange region of two p13suc1 dimers from the P212121 asymmetric unit (yellow and blue) with p13or (red). In p13or, two ordered water molecules, related by twofold symmetry, are present. Each dimer from the space group P212121 has only one water molecule in this region. (Panels (a) and (b) generated with the program Raster3D [38]; panel (c) generated with MOLSCRIPT [37].) Structure 1996 4, 299-309DOI: (10.1016/S0969-2126(96)00034-2)

Figure 6 Comparison of the strand-exchange region of p13or with the corresponding loop in p13hex. Residues in p13or and in its strand-exchange partner are shown in grey and white, respectively. The corresponding loop in p13hex is shown in black. (This figure was generated using MOLSCRIPT [37].) Structure 1996 4, 299-309DOI: (10.1016/S0969-2126(96)00034-2)

Figure 7 Comparison of conserved surface patches in p13or and p13hex. The conserved hydrophobic patch is shown in orange, and the positively charged patch in purple for (a) p13hex [19] and (b) p13or. The CHAPS molecule is shown in green with the oxygen atoms in red. The molecular symmetry twofold axis is vertical in this view. (Figure generated with the program GRASP [39].) Structure 1996 4, 299-309DOI: (10.1016/S0969-2126(96)00034-2)

Figure 7 Comparison of conserved surface patches in p13or and p13hex. The conserved hydrophobic patch is shown in orange, and the positively charged patch in purple for (a) p13hex [19] and (b) p13or. The CHAPS molecule is shown in green with the oxygen atoms in red. The molecular symmetry twofold axis is vertical in this view. (Figure generated with the program GRASP [39].) Structure 1996 4, 299-309DOI: (10.1016/S0969-2126(96)00034-2)

Figure 8 Superposition of p13hex and p13or. The asymmetric unit of p13or (red) is superimposed on subunit A of p13hex (blue) [19]. Also shown is a symmetry-related monomer of p13or (green), which illustrates that a similar interface exists in both crystal forms. (Figure generated with the program Raster3D [38].) Structure 1996 4, 299-309DOI: (10.1016/S0969-2126(96)00034-2)

Figure 9 Electron density for CHAPS. 2Fo–Fc, 1σ electron density and the CHAPS molecule from the current model. Only the first four carbons of the detergent tail are defined in the electron-density map. The complete structure of the detergent tail is -C20(CH3)(CH2)2CONH(CH2)3N+(CH3)2(CH2)3SO3−. Structure 1996 4, 299-309DOI: (10.1016/S0969-2126(96)00034-2)