Maik Goette, Martin C. Stumpe, Ralf Ficner, Helmut Grubmüller 

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Molecular Determinants of Snurportin 1 Ligand Affinity and Structural Response upon Binding  Maik Goette, Martin C. Stumpe, Ralf Ficner, Helmut Grubmüller  Biophysical Journal  Volume 97, Issue 2, Pages 581-589 (July 2009) DOI: 10.1016/j.bpj.2009.04.049 Copyright © 2009 Biophysical Society Terms and Conditions

Figure 1 Basic nucleocytoplasmatic shuttling cycle of snRNA. In the nucleus, an export complex (red) is formed, which binds to the m7G-capped snRNA and transports it through the nuclear pore complex (NPC). After dissociation, Sm-core assembly, and cap hypermethylation, the import complex (purple and green) is formed by association of the UsnRNP complex with importin-β and snurportin 1 (SPN1), which binds the m3G-capped snRNA and the survival motor neuron complex. After transport into the nucleus, the import complex dissociates, and the UsnRNP is fully assembled. Biophysical Journal 2009 97, 581-589DOI: (10.1016/j.bpj.2009.04.049) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 2 Chemical and crystal structures. (A) m3GpppG (state A), (B) m7GpppG (state B). The difference of both molecules is shown in the gray ellipsoids, where A represents the N2-nitrogen in the hypermethylated and B in the nonmethylated state. (C) Human snurportin 1 with bound m3GpppG ligand (PDB ID:1XK5). The α-helices are colored in red, β-sheets in green and loop-regions are colored in gray. m3GpppG is shown in a ball-and-stick model. Biophysical Journal 2009 97, 581-589DOI: (10.1016/j.bpj.2009.04.049) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 3 (A) Gaussian work distribution of 50 calculated work values for morphing m3GpppG into m7GpppG (λ0→1) and m7GpppG into m3GpppG (λ1→0). The intersection point of both Gaussians describes the value with zero dissipative work. (B) Thermodynamic cycle. ΔG3 and ΔG4 are calculated via thermodynamic integration simulations. ΔΔG = ΔG1-ΔG2 = ΔG3-ΔG4. Biophysical Journal 2009 97, 581-589DOI: (10.1016/j.bpj.2009.04.049) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 4 Root mean-square deviations (RMSD). (A) Backbone RMSD of SPN1 with and without m3GpppG as ligand. The black curve denotes the RMSD of ligand-bound SPN1. The remaining curves represent the RMSDs of six independent trajectories of snurportin 1 in absence of the ligand. The trajectories with the highest RMSD are shown in red and blue; the most stable trajectory is shown in green. (B) Time-resolved amino acid RMSDs of SPN1 bound to m3GpppG-cap. (C) The ligand free protein, where the RMSD from all six trajectories was averaged. The first 10 amino acids from each terminus have been removed in this analysis. For a better resolution in the lower RMSD regions, all values above 4 Å have been truncated to this value. RMSF and time-averaged RMSD are shown for comparison above the respective plots. Biophysical Journal 2009 97, 581-589DOI: (10.1016/j.bpj.2009.04.049) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 5 Color-coded structure of SPN1. Selected high RMSD amino acids from the ligand free SPN1 trajectories are colored according to their position in the structure. (Blue) C-terminal domain; (red) β 10-related region; (green) loop region; (yellow) Lys144-loop; (Pink) N-terminus; (light blue) C-terminus; and (transparent) m3GpppG (for guidance). Biophysical Journal 2009 97, 581-589DOI: (10.1016/j.bpj.2009.04.049) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 6 PCA of snurportin 1. The black cloud represents the 650-ns trajectory of the protein with m3GpppG ligand bound, projected onto the first two eigenvectors, and the yellow square as the general starting configuration. The clouds colored in red, green, and blue display the trajectories 1, 2, and 6 of the protein without ligand as in Fig. 4A. Every 10th frame of the respective trajectories has been used in the projections. (Inset) The first 10 eigenvectors of the covariance matrix. The dashed line is the cumulative sum of the contribution to the total fluctuations. The first two eigenvectors describe 49% of the main global motion. Biophysical Journal 2009 97, 581-589DOI: (10.1016/j.bpj.2009.04.049) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 7 Snapshots of the binding pocket and C-terminus of SPN1 at 0, 79.7, and 148 ns. (A) Trp107 and Trp276 are shown in orange; the residues Cys124, Ile175, Leu186, and Leu258, building a hydrophobic pocket, in black; Arg129 and Lys144 in blue; and Asp173 in red. The β-strand 1 is colored purple. (B) Val111 (yellow), Leu115 (orange), Val282 (red), Val285 (blue), and Leu286 (light blue). Biophysical Journal 2009 97, 581-589DOI: (10.1016/j.bpj.2009.04.049) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 8 Three-dimensional density distribution of water molecules around the m3GpppG and m7GpppG ligands. (A and B) The m3G-nucleoside in water and complexed to SPN1; (C and D) the m7G-nucleoside. (Left column) Fifteen-percent of the total solvation shell, starting from the highest to lower densities, as a qualitative isosurface view. (Right column) Sixty-percent of the density in a quantitative plot. For clarity of presentation, a logarithmic color scale was chosen. Biophysical Journal 2009 97, 581-589DOI: (10.1016/j.bpj.2009.04.049) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 9 Root mean-square deviations of Trp107. The RMSD curves were smoothed with a running average, where 100 data points where used for averaging. The coloring indicates the deviation of Trp107 in trajectories with m7GpppG, where green represents a small, blue a medium, and red a strong deviation. Black shows the deviation of Trp107 with m3GpppG. Biophysical Journal 2009 97, 581-589DOI: (10.1016/j.bpj.2009.04.049) Copyright © 2009 Biophysical Society Terms and Conditions