18 research outputs found

    Binding of an RNA pol II Ligand to the WW Domain of Pin1 Using Molecular Dynamics Docking Simulations

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    A novel docking protocol using a long, all atom molecular dynamics (MD) simulation, in an explicit solvent medium, without using any distance constraints is presented. This MD docking protocol is able to dock ligands, based on the C-terminal domain (CTD) of RNA polymerase II, into the tryptophan-tryptophan (WW) domain of Pin1. In this docking process, a significant loop-bending event occurs in order to encircle the ligand into its solvent exposed binding site, which cannot be simulated using current protocols. The simulations were validated structurally and energetically against an X-ray structure to confirm correct sampling of conformational space. Based on these simulations, and justification of the starting structure as a valid intermediate structure, a potential molecular basis for binding was predicted as well as confirming the key residues involved in the formation of the final strong and stable Pin1 WW domain-ligand complex

    Binding of an RNA pol II Ligand to the WW Domain of Pin1 Using Molecular Dynamics Docking Simulations

    No full text
    A novel docking protocol using a long, all atom molecular dynamics (MD) simulation, in an explicit solvent medium, without using any distance constraints is presented. This MD docking protocol is able to dock ligands, based on the C-terminal domain (CTD) of RNA polymerase II, into the tryptophan-tryptophan (WW) domain of Pin1. In this docking process, a significant loop-bending event occurs in order to encircle the ligand into its solvent exposed binding site, which cannot be simulated using current protocols. The simulations were validated structurally and energetically against an X-ray structure to confirm correct sampling of conformational space. Based on these simulations, and justification of the starting structure as a valid intermediate structure, a potential molecular basis for binding was predicted as well as confirming the key residues involved in the formation of the final strong and stable Pin1 WW domain-ligand complex

    Summary data for individual β9-strand mutants.

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    <p>(A) Scatter plot of the V<sub>0.5</sub> values for the 3 s isochronal activation (open symbols) and 3 s isochronal deactivation (closed symbols) for WT (black), AAA (grey), F860A (red), N861A (magenta), L862A (blue), F860L (orange), F860Y (green) and F860R (cyan). (B) Scatter plot of the V<sub>0.5</sub> values for the steady-state inactivation (open symbols) for WT, AAA, F860A, N861A, L862A, F860L, F860Y and F860R (same colour scheme as in panel A). In all panels, the mean and SEM are indicated by horizontal bars and asterisks indicate values that are statistically significantly different to WT (<i>P</i><0.05, ANOVA). The dashed horizontal lines indicate mean values for WT. The values for all mutants are summarized in Table S1 in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0077032#pone.0077032.s001" target="_blank">File S1</a>.</p

    Topology of Kv11.1 channels and sequence analysis of cNBH domains.

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    <p>(A) Topology of Kv11.1 channel showing the intracellular N-terminal PAS domain (blue), transmembrane voltage sensing domain (green), pore domain (yellow) and intracellular C-terminal C-linker and cNBH domains (orange). Inset shows the homology model of the cNBH domain of Kv11.1 generated based on the mEAG crystal structure <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0077032#pone.0077032-MarquesCarvalho1" target="_blank">[13]</a>. (B) Sequence alignment of mHCN2, zELK, mEAG and human Kv11.1 extracted from a Clustalw alignment of the entire family of KCNHx/HCNx/CNGx ion channels. Sequences shown correspond to the dotted box region shown in panel A. Sequence similarity to the Kv11.1 are marked by white text/red box (identical) and black text/yellow box (similar). Non-conserved sequences are in grey. Clear rods and arrows represent the consensus α-helices and β-strands while filled rods and arrows indicate the differences with orange, green and blue representing mHCN2, zELK and mEAG, respectively. The hydrogen bond between asparagine (arrow) and tyrosine (asterisk) in zELK is not observed in the others.</p

    Sequence alignment and structure of hERG S4–S5 linker.

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    <p>A. Sequence alignment of hERG and Kv1.2 for the distal S4, S4–S5 linker and proximal S5 domains. The leucine residues (red) of Kv1.2 S4–S5 linker correspond to tyrosine and valine residues in hERG. Glycine residue (green) in both channels is also conserved. B. Chemical shift index (CSI) plot for NMR structure of hERG S4–S5. CSI values less than −0.1 ppm are indicative of α-helical structure. C. 20 lowest energy structures for hERG S4–S5 with side chains colour coded according to physiochemical properties (basic: blue, acidic: red, polar: green, aromatic: yellow, hydrophobic: grey).</p

    Trafficking assay of LQT2 mutants located within β9-strand.

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    <p>(A) Typical western blot of WT, N861I and N861H mutant channels. WT shows two bands at ∼155 kDa and ∼135 kDa. The ∼155 kDa band disappears following digestion of surface proteins with proteinase K. The N861H mutant shows only a single ∼135 kDa band. N861I contains both ∼155 kDa and ∼135 kDa bands. Arrow indicates degradation band after proteinase K digestion. (B) Normalized expression levels of N861H and N861I relative to WT for the fully glycosylated (∼155 kDa band) and core-glycosylated (∼135 kDa band) proteins. (C) The partially trafficking defective N861I can be rescued by incubation with cisparide whereas N861H was not rescued by cisapride. (D) Co-imunpreciptation of HA-tagged mutant subunits with Flag-tagged WT subunits. (E) Top panel: Summary of 3 s isochronal activation V<sub>0.5</sub> (open symbols) and 3 s isochronal deactivation V<sub>0.5</sub> (closed symbols) for WT (black), N861H (magenta) and N861I (blue). Asterisks indicate <i>P</i><0.05 (ANOVA) compared to WT. Bottom panel: Summary of the V<sub>0.5</sub> of steady-state inactivation for WT, N861H and N861I (same colours as in top panel). Mean data for all mutants are summarized in Table S1 in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0077032#pone.0077032.s001" target="_blank">File S1</a>.</p

    Secondary structure prediction and MD simulations of cNBH domain.

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    <p>Sequence prediction of the cNBH domain around the β9-strand for (A) WT (i) and AAA mutant (ii). (B) RMSD (i) and RMSF (ii) of WT (red) and AAA mutant (black) from the 60 ns of MD simulations. The blue box highlights the most significant difference between WT and AAA mutant in the backbone fluctuation. (C) The structures that have the lowest structural fluctuation to the centroid structure in the most populated cluster from the last 10 ns for WT (i) and AAA mutant (ii). Residues involved in hydrophobic interactions, defined by being within 4 Å of residues 860, 861 and 862 (cyan), are highlighted in magenta for WT (i) and AAA mutant (ii). There are reduced hydrophobic interactions in the AAA mutant. (D) Summary of residues that participate in hydrogen bonds with residues 860, 861 and 862 in WT (i) and the AAA mutant (ii) that are present for more than 5% of the 60 ns of MD simulation (see <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0077032#pone-0077032-t001" target="_blank">Table 1</a> for details).</p

    Inactivation phenotype of AAA mutant.

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    <p>(A) Current traces correspond to dotted box in the voltage protocol used to measure the recovery of inactivation for (i) WT and (ii) AAA mutant. Current traces recorded at −80 mV are highlighted to show the faster recovery of inactivation for AAA mutant. (B) Current traces correspond to dotted box in the voltage protocol used to measure the onset of inactivation for (i) WT and (ii) AAA mutant. Current traces recorded at 0 mV are highlighted to show the slower onset of inactivation for the AAA mutant. (C) Summary of rates of recovery and onset of inactivation plotted against voltages between −130 and +50 mV. The data points for −80 and 0 mV are indicated by the arrows. The mid-point of steady-state inactivation for the AAA mutant (grey) is right-shifted by ∼33 mV from WT (black). (D) V<sub>0.5</sub> of steady-state inactivation for WT (−51.7±1.9 mV, n = 7; filled black circle) and AAA mutant (−18.7±2.7 mV, n = 4; filled gray circle) (*indicates p<0.05 versus WT, ANOVA). Data are presented as mean ± SEM.</p

    Gating Phenotype of AAA mutant.

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    <p>(A) Family of current traces recorded during a 3 s isochronal activation protocol for (i) WT and (ii) AAA mutant channels. (iii) Isochronal activation curves for WT (filled black circle) and AAA mutant (filled grey circle). The mean V<sub>0.5</sub> of isochronal activation for the AAA mutant and WT were −15.1±1.0 mV (n = 4) and −23.1±0.4 mV (n = 4), respectively; see Table S1 in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0077032#pone.0077032.s001" target="_blank">File S1</a>. (B) Families of −70 mV tail current traces recorded during a 3 s isochronal deactivation protocol for (i) WT and (ii) AAA mutant. The dotted box in the voltage protocol indicates the portion of the traces shown in the current recordings. (iii) Isochronal deactivation curves for WT (filled black circle) and AAA mutant (filled grey circle). Data are presented as mean ± SEM for n = 4 experiments. The mean V<sub>0.5</sub> of isochronal deactivation for the AAA mutant and WT were −23.4±1.1 mV (n = 4) and −61.3±0.8 mV (n = 4), respectively. (C) Typical family of current traces recorded between −60 to −160 mV at 20 mV intervals, corresponding to the dotted box in the voltage protocol, used to measure rates of deactivation for (i) WT and (ii) AAA mutant. (iii) Summary of the rates of deactivation for AAA mutant (grey) and WT (black). Data shown as mean ± SEM (n = 4), error bars are within the symbols.</p
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