Hinge-Like Motions in RNA Kink-Turns: The Role of the Second A-Minor Motif and Nominally Unpaired Bases  Filip Rázga, Jaroslav Koča, Jiří Šponer, Neocles.

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Hinge-Like Motions in RNA Kink-Turns: The Role of the Second A-Minor Motif and Nominally Unpaired Bases  Filip Rázga, Jaroslav Koča, Jiří Šponer, Neocles B. Leontis  Biophysical Journal  Volume 88, Issue 5, Pages 3466-3485 (May 2005) DOI: 10.1529/biophysj.104.054916 Copyright © 2005 The Biophysical Society Terms and Conditions

Figure 1 Schematic drawings of K-turn motifs with annotations to indicate non-WC basepairs (Leontis and Westhof, 2001). Circles represent WC edges, squares Hoogsteen-edges, and triangles Sugar-edges. Open symbols indicate trans pairing and closed symbols indicate cis pairing. Boldface shaded font indicates nucleotide in syn conformation and shaded arrows indicate directional changes in the sugar-phosphate backbones. (a) U4 snRNA. (b) Simulated Kt-38 from 23S rRNA of H. marismortui. (c) Simulated Kt-42 from 23S rRNA of H. marismortui. (d) Simulated Kt-58 from 23S rRNA of H. marismortui. The U4 snRNA K-turn is in full agreement with the consensus K-turn sequence (cf. Supplementary Material, Fig. S1). Biophysical Journal 2005 88, 3466-3485DOI: (10.1529/biophysj.104.054916) Copyright © 2005 The Biophysical Society Terms and Conditions

Figure 2 Observed variability of the second A-minor interhelical interaction in the K-turns involving the second conserved adenosine of the NC-stem and the first basepair of the C-stem. (a) Direct H-bonding A-minor type I interaction in Kt-77 from T. thermophilus 23S rRNA (Nikulin et al., 2003). (b) Water-inserted A-minor type I interaction (H. marismortui 23S rRNA, Kt-7). (c) A-minor type 0 interaction (H. marismortui 23S rRNA, Kt-46). Biophysical Journal 2005 88, 3466-3485DOI: (10.1529/biophysj.104.054916) Copyright © 2005 The Biophysical Society Terms and Conditions

Figure 3 Normalized histograms of interatomic distances involving the second conserved adenosine in the NC-stem and the cytosine of the first basepair of the C-stem in simulations of Kt-38 (left) and Kt-42 (right). Vertical lines indicate values in the crystal structure of the H. marismortui 50S subunit. Biophysical Journal 2005 88, 3466-3485DOI: (10.1529/biophysj.104.054916) Copyright © 2005 The Biophysical Society Terms and Conditions

Figure 4 Normalized histograms of A/G C1′-C1′ distances in the second A-minor interaction in Kt-38 and Kt-42 simulations. The vertical lines indicate the respective x-ray values. The trans SE/SE basepairs A1032/G940 in Kt-38 and A1152/G1216 in Kt-42 are stable and act as fulcra for the motion. The pivoting motion then produces significant fluctuations in the A(O2′)-C(O2) and A(C1′)-C(C1′) distances in the second basepair of this A-minor interaction, i.e., A1032/C1026 in Kt-38 and A1152/C1147 in Kt-42 (see Fig. 3). Biophysical Journal 2005 88, 3466-3485DOI: (10.1529/biophysj.104.054916) Copyright © 2005 The Biophysical Society Terms and Conditions

Figure 5 Stereo view of hydrogen-bonding and hydration patterns of the second A-minor interaction observed in simulations of Kt-38 and Kt-42. (a) Closed state: A(O2′) is directly H-bonded to C(O2) and C(O2′). (b) Semiclosed state: a long-residency water molecule donates H-bond to C(O2) and accepts an H-bond from A(O2′). (c) Semiopen state: the water molecule donates H-bonds to both C(O2) and A(O2′). (d) Open state: a second water molecule mediates the A(O2′)-C(O2′) interaction. Biophysical Journal 2005 88, 3466-3485DOI: (10.1529/biophysj.104.054916) Copyright © 2005 The Biophysical Society Terms and Conditions

Figure 6 Superposition of 3D structures of closed and open structures for (a) Kt-38 and (b) Kt-42. The crystallographic structures are shown in black (open for Kt-38 and closed for Kt-42, see text) and representative simulated structures are shaded. (c) Normalized histograms of the interhelical angles calculated as described in the Methods section. The asymmetric shape of these distributions corresponds to open/closed dynamics of Kt-38 and Kt-42. The vertical lines indicate the x-ray values. Biophysical Journal 2005 88, 3466-3485DOI: (10.1529/biophysj.104.054916) Copyright © 2005 The Biophysical Society Terms and Conditions

Figure 7 (a) The long-residency hydration site between A1032(N6) and G938(N3). (b) Stabilization of the C1213/A1154 basepair via interaction of Na+ ions with both its groove edges. Biophysical Journal 2005 88, 3466-3485DOI: (10.1529/biophysj.104.054916) Copyright © 2005 The Biophysical Society Terms and Conditions

Figure 8 Schematic comparison of the initial Kt-58 structure with the second conformation formed after a few nanoseconds of simulation and persisting for the rest of the simulation. For annotations, see Fig. 1. Biophysical Journal 2005 88, 3466-3485DOI: (10.1529/biophysj.104.054916) Copyright © 2005 The Biophysical Society Terms and Conditions

Figure 9 Superposition of 3D structures of initial and final structures of (a) Kt-58 and (b) Kt-U4. The x-ray structures are shown in blue (more bent for Kt-58 and more open for Kt-U4) and representative final structures (averaged from MD; step, 500ps) in red. The C-stem is overlaid. The changes from initial to final geometry were permanent in the simulated timescale (PDB files are available in Supplementary Material). Biophysical Journal 2005 88, 3466-3485DOI: (10.1529/biophysj.104.054916) Copyright © 2005 The Biophysical Society Terms and Conditions

Figure 10 Main conformational change of the kink in simulation of the Kt-U4 leading to a decrease of the interhelical angle. Initial (a) and final (b) geometry of the core nucleotides localized in the K region. Stacked residues (A30 shaded) are marked by arrows. Biophysical Journal 2005 88, 3466-3485DOI: (10.1529/biophysj.104.054916) Copyright © 2005 The Biophysical Society Terms and Conditions