Christopher Wostenberg, W.G. Noid, Scott A. Showalter 

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MD Simulations of the dsRBP DGCR8 Reveal Correlated Motions that May Aid pri- miRNA Binding  Christopher Wostenberg, W.G. Noid, Scott A. Showalter  Biophysical Journal  Volume 99, Issue 1, Pages 248-256 (July 2010) DOI: 10.1016/j.bpj.2010.04.010 Copyright © 2010 Biophysical Society Terms and Conditions

Figure 1 (A) Schematic representation of the primary sequence of DGCR8. (B) A ribbon diagram representing the crystal structure of DGCR8 Core (PDB 2YT4, residues 505–701) shows a well-structured linker (H3 and H4) and a C-terminal helix (H5, black). The nomenclature used is the same as the crystal structure nomenclature (20). dsRBD1 is shown in red and dsRBD2 is shown in green (in dsRBD2, helices and strands are denoted with primes to indicate equivalence with secondary structures to dsRBD1). The arrows indicate the proposed dsRNA-binding sites. Biophysical Journal 2010 99, 248-256DOI: (10.1016/j.bpj.2010.04.010) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 2 RMSD traces show the overall stability of the dsRBDs during the MD simulations and highlight the rearrangement of the domains relative to each other in the Core simulation. (A) RMSD traces of dsRBD1 (red), dsRBD2 (green), and Core (black) relative to the starting crystal structure. (B) RMSD trace of the isolated dsRBD1 (red) compared with the RMSD trace of dsRBD1 from the Core simulation (gray). (C) RMSD trace of the isolated dsRBD2 (green) compared with the RMSD trace of dsRBD2 from the Core simulation (gray). In both B and C the total Core RMSD (black) is given as a reference. (D) Ribbon bundle from the Core simulation in which dsRBD1 (red) is superimposed. (E) Ribbon bundle from the Core simulation in which dsRBD2 (green) is superimposed. Both bundles are created by taking structures from the simulation every 50 ns. Biophysical Journal 2010 99, 248-256DOI: (10.1016/j.bpj.2010.04.010) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 3 Ribbon diagrams spanning the range of motion in the largest-amplitude ANM illustrate the correlated movement of the dsRBD wings toward each other. Colorized regions highlight the sections of maximal displacement, with dsRBD1 and dsRBD2 colored identically in the given structure to guide the eye. Biophysical Journal 2010 99, 248-256DOI: (10.1016/j.bpj.2010.04.010) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 4 Cα correlation matrices reveal the collective backbone motions of isolated dsRBD1 (A), isolated dsRBD2 (B), dsRBD1 from the Core simulation (C), and dsRBD2 from the Core simulation (D). To highlight differences between the collective dynamics of the domains in isolation and in the Core, a difference matrix between panels A and C or panels B and D is shown below the diagonal in panels C and D, respectively. The color bar on the right shows the color scale indicating strong positive correlation (red), strong negative correlation (blue), and noncorrelated motion (green) used in the figure. Biophysical Journal 2010 99, 248-256DOI: (10.1016/j.bpj.2010.04.010) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 5 IDE analysis reveals motions correlating the conformations of dsRBD1 and dsRBD2 in the Core. (A) Mode collectivity plotted as a function of the eigenvalue for each mode reveals the separation of motion into three global reorientational modes (upper right) and the N-3 internal modes. (B) The IDE matrix from the Core simulation is represented by its cross-correlation coefficients (upper triangle), demonstrating the anticorrelated nature of the global reorientation of the two dsRBDs with respect to each other. Subtracting the contributions from the three global modes before constructing the cross-correlation coefficients preserves only the effects of internal dynamics (lower triangle). The color bar on the right shows the color scale indicating strong positive correlation (red), strong negative correlation (blue), and noncorrelated motion (green) used in the figure. Biophysical Journal 2010 99, 248-256DOI: (10.1016/j.bpj.2010.04.010) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 6 Ribbon diagrams spanning the range of motion sampled by projecting the limiting excursions along the largest-amplitude internal eigenmode of the IDE matrix onto the starting crystal structure. Colorized regions highlight the sections of maximal displacement, with dsRBD1 and dsRBD2 colored identically in the given structure to guide the eye. Biophysical Journal 2010 99, 248-256DOI: (10.1016/j.bpj.2010.04.010) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 7 Expanded views of the Core crystal structure showing the interfacial interactions between dsRBD1 (red) and dsRBD2 (green). Stabilization of the interface comes from (A) multiple hydrogen bonds formed between the C-terminal helix and either dsRBD1 or dsRBD2; (B) a variety of packing interactions, including a hydrogen bond between Asn-631 and Gly-550; and (C) a salt bridge between Asp-549 and Lys-659. All distances shown are between the indicated pair of atoms in the crystal structure. Their variation in the MD simulations is discussed in the text. Biophysical Journal 2010 99, 248-256DOI: (10.1016/j.bpj.2010.04.010) Copyright © 2010 Biophysical Society Terms and Conditions