Mechanism and Energetics of Charybdotoxin Unbinding from a Potassium Channel from Molecular Dynamics Simulations  Po-chia Chen, Serdar Kuyucak  Biophysical.

Slides:



Advertisements
Similar presentations
Molecular Analysis of the Interaction between Staphylococcal Virulence Factor Sbi-IV and Complement C3d  Ronald D. Gorham, Wilson Rodriguez, Dimitrios.
Advertisements

A Protein Dynamics Study of Photosystem II: The Effects of Protein Conformation on Reaction Center Function  Sergej Vasil’ev, Doug Bruce  Biophysical.
Volume 109, Issue 7, Pages (October 2015)
The Protonation State of the Glu-71/Asp-80 Residues in the KcsA Potassium Channel: A First-Principles QM/MM Molecular Dynamics Study  Denis Bucher, Leonardo.
Hydroxide and Proton Migration in Aquaporins
Vishwanath Jogini, Benoît Roux  Biophysical Journal 
Shaogui Wu, Laicai Li, Quan Li  Biophysical Journal 
Ion Permeation through a Narrow Channel: Using Gramicidin to Ascertain All-Atom Molecular Dynamics Potential of Mean Force Methodology and Biomolecular.
Volume 83, Issue 3, Pages (September 2002)
Ching-Hsing Yu, Samuel Cukierman, Régis Pomès  Biophysical Journal 
Molecular Dynamics Free Energy Calculations to Assess the Possibility of Water Existence in Protein Nonpolar Cavities  Masataka Oikawa, Yoshiteru Yonetani 
Influence of Chain Length and Unsaturation on Sphingomyelin Bilayers
Jing Han, Kristyna Pluhackova, Tsjerk A. Wassenaar, Rainer A. Böckmann 
A Model of H-NS Mediated Compaction of Bacterial DNA
Fangqiang Zhu, Emad Tajkhorshid, Klaus Schulten  Biophysical Journal 
Elucidating the Locking Mechanism of Peptides onto Growing Amyloid Fibrils through Transition Path Sampling  Marieke Schor, Jocelyne Vreede, Peter G.
Po-Chao Wen, Emad Tajkhorshid  Biophysical Journal 
Volume 92, Issue 1, Pages (January 2007)
Michel A. Cuendet, Olivier Michielin  Biophysical Journal 
Mechanism of the αβ Conformational Change in F1-ATPase after ATP Hydrolysis: Free- Energy Simulations  Yuko Ito, Mitsunori Ikeguchi  Biophysical Journal 
Christian Kappel, Ulrich Zachariae, Nicole Dölker, Helmut Grubmüller 
Coarse-Grained Peptide Modeling Using a Systematic Multiscale Approach
Exterior Site Occupancy Infers Chloride-Induced Proton Gating in a Prokaryotic Homolog of the ClC Chloride Channel  David L. Bostick, Max L. Berkowitz 
Volume 98, Issue 8, Pages (April 2010)
G. Fiorin, A. Pastore, P. Carloni, M. Parrinello  Biophysical Journal 
A Molecular Dynamics Study of Ca2+-Calmodulin: Evidence of Interdomain Coupling and Structural Collapse on the Nanosecond Timescale  Craig M. Shepherd,
Dániel Szöllősi, Gergely Szakács, Peter Chiba, Thomas Stockner 
Volume 89, Issue 3, Pages (September 2005)
J.L. Robertson, L.G. Palmer, B. Roux  Biophysical Journal 
Volume 96, Issue 7, Pages (April 2009)
Ligand Binding to the Voltage-Gated Kv1
Modeling Diverse Range of Potassium Channels with Brownian Dynamics
Li Sun, Jeffrey K. Noel, Herbert Levine, José N. Onuchic 
Simone Furini, Carmen Domene  Biophysical Journal 
Volume 102, Issue 9, Pages (May 2012)
Validating Solution Ensembles from Molecular Dynamics Simulation by Wide-Angle X- ray Scattering Data  Po-chia Chen, Jochen S. Hub  Biophysical Journal 
Sequential Unfolding of Individual Helices of Bacterioopsin Observed in Molecular Dynamics Simulations of Extraction from the Purple Membrane  Michele.
Molecular Dynamics Study of the KcsA Potassium Channel
Sundeep S. Deol, Peter J. Bond, Carmen Domene, Mark S.P. Sansom 
Volume 108, Issue 10, Pages (May 2015)
Absence of Ion-Binding Affinity in the Putatively Inactivated Low-[K+] Structure of the KcsA Potassium Channel  Céline Boiteux, Simon Bernèche  Structure 
Zara A. Sands, Alessandro Grottesi, Mark S.P. Sansom 
Volume 107, Issue 5, Pages (September 2014)
Activation of the Edema Factor of Bacillus anthracis by Calmodulin: Evidence of an Interplay between the EF-Calmodulin Interaction and Calcium Binding 
Volume 103, Issue 5, Pages (September 2012)
Cholesterol Modulates the Dimer Interface of the β2-Adrenergic Receptor via Cholesterol Occupancy Sites  Xavier Prasanna, Amitabha Chattopadhyay, Durba.
Protein Grabs a Ligand by Extending Anchor Residues: Molecular Simulation for Ca2+ Binding to Calmodulin Loop  Chigusa Kobayashi, Shoji Takada  Biophysical.
Tsuyoshi Terakawa, Shoji Takada  Biophysical Journal 
Velocity-Dependent Mechanical Unfolding of Bacteriorhodopsin Is Governed by a Dynamic Interaction Network  Christian Kappel, Helmut Grubmüller  Biophysical.
Kristen E. Norman, Hugh Nymeyer  Biophysical Journal 
Volume 112, Issue 12, Pages (June 2017)
Open-State Models of a Potassium Channel
Michel A. Cuendet, Olivier Michielin  Biophysical Journal 
The Selectivity of K+ Ion Channels: Testing the Hypotheses
Coupling of S4 Helix Translocation and S6 Gating Analyzed by Molecular-Dynamics Simulations of Mutated Kv Channels  Manami Nishizawa, Kazuhisa Nishizawa 
Michael Thomas, Dylan Jayatilaka, Ben Corry  Biophysical Journal 
Coupling of S4 Helix Translocation and S6 Gating Analyzed by Molecular-Dynamics Simulations of Mutated Kv Channels  Manami Nishizawa, Kazuhisa Nishizawa 
Mechanism of Anionic Conduction across ClC
Alternative Mechanisms for the Interaction of the Cell-Penetrating Peptides Penetratin and the TAT Peptide with Lipid Bilayers  Semen Yesylevskyy, Siewert-Jan.
OmpT: Molecular Dynamics Simulations of an Outer Membrane Enzyme
Membrane Insertion of a Voltage Sensor Helix
Volume 95, Issue 7, Pages (October 2008)
Mechanism of Interaction between the General Anesthetic Halothane and a Model Ion Channel Protein, III: Molecular Dynamics Simulation Incorporating a.
Volume 114, Issue 2, Pages (January 2018)
Sebastian Fritsch, Ivaylo Ivanov, Hailong Wang, Xiaolin Cheng 
Chze Ling Wee, David Gavaghan, Mark S.P. Sansom  Biophysical Journal 
Christian Kappel, Ulrich Zachariae, Nicole Dölker, Helmut Grubmüller 
Volume 78, Issue 6, Pages (June 2000)
Volume 94, Issue 11, Pages (June 2008)
Volume 98, Issue 4, Pages (February 2010)
Presentation transcript:

Mechanism and Energetics of Charybdotoxin Unbinding from a Potassium Channel from Molecular Dynamics Simulations  Po-chia Chen, Serdar Kuyucak  Biophysical Journal  Volume 96, Issue 7, Pages 2577-2588 (April 2009) DOI: 10.1016/j.bpj.2008.12.3952 Copyright © 2009 Biophysical Society Terms and Conditions

Figure 1 NMR structure of ChTX from two different perspectives. (A) View from the top, as it is docked in the KcsA channel. The three disulfide bonds that confer some rigidity to ChTX are clearly visible (indicated by yellow). (B) Side view, where the arginine and lysine residues involved in the binding are indicated. Visual figures in this article have been rendered using Tachyon (Tachyon Software, Denver, CO) within the VMD environment. Biophysical Journal 2009 96, 2577-2588DOI: (10.1016/j.bpj.2008.12.3952) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 2 Side view of ChTX in complex with a KcsA potassium channel surrogate. ChTX backbone is shown in yellow and the side chains of K11′, K27′, R25′, and R34′ residues involved in the binding are explicitly shown. Two of the four monomers in KcsA (B and D) are shown clearly. The monomer A is removed and C is shown as a shadow for clarity. The carbonyl groups in the filter and the side chains of D80 and D64 residues are explicitly indicated. The water molecules in the filter and two K+ ions (one at the S4 binding site and one in the cavity) are also shown. Biophysical Journal 2009 96, 2577-2588DOI: (10.1016/j.bpj.2008.12.3952) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 3 The RMSD of ChTX in bulk water, in complex with the KcsA channel, and in the last umbrella sampling window (top). The NMR structure 2CRD1 is used as the reference state. RMSD of the surface residues of KcsA (i.e., 49–64 in S5-P and 78–87 in F-S6) with and without ChTX bound (bottom). The NMR structure of the complex 2A9H is used as the reference state. Biophysical Journal 2009 96, 2577-2588DOI: (10.1016/j.bpj.2008.12.3952) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 4 Distributions of the distances between the strongly interacting pairs in the KcsA channel-ChTX complex. The K27′-Y78 histogram shows the N-O distances for each of the four monomers denoted by A–D. Three H atoms in the amide group make hydrogen bonds with the carbonyls of A, B, and D, while that of C is left free. The elongated tail in the R34′-D80 plot stems from equilibration—this interaction is established shortly after system equilibration and remains associated for the rest of the simulation. Biophysical Journal 2009 96, 2577-2588DOI: (10.1016/j.bpj.2008.12.3952) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 5 Convergence study of the PMF. Data from the first 11 Å is used as a guide to check for sufficient convergence. Here, vertical axis refers to the estimated PMF, and horizontal axis, z, refers to the COM position of the ChTX backbone heavy-atoms, with z = 0 defined as the center of the simulation box (this convention holds throughout the article). The binding site is located at z ∼ 31 Å measured along the channel axis. The last 3.2 ns of the MD data is divided into eight equal parts and a PMF is constructed from each set. The PMFs are sequentially numbered from 1 to 8, as indicated in the figure. Biophysical Journal 2009 96, 2577-2588DOI: (10.1016/j.bpj.2008.12.3952) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 6 Effect of increasing the number of windows on the PMF. The density data used in Fig. 5 are augmented by including extra windows at 0.25 Å intervals, up to z ∼ 36 Å as shown by the dotted lines. The window number and positions are indicated in the figure. The resulting PMF (solid line), is compared to the first one obtained using 0.5 Å intervals (dashed line). Biophysical Journal 2009 96, 2577-2588DOI: (10.1016/j.bpj.2008.12.3952) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 7 Comparison of the PMFs obtained from the umbrella sampling simulations using the force constants of 20 kcal/mol/Å2 (solid line) and 40 kcal/mol/Å2 (dashed line). The same routine employed in the construction of the k-20 PMF has been used for the k-40 PMF. (Inset) Distribution of the ChTX-COM as overlapping histograms along the reaction coordinate. For each window, we display the actual distribution of the ChTX-COM (shaded histogram) and its constraint coordinate (dotted line, usually to the right). (Solid curve) Distribution for the extra window (to cover the poorly sampled region, see Methods). Biophysical Journal 2009 96, 2577-2588DOI: (10.1016/j.bpj.2008.12.3952) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 8 Comparison of the NMR structure of ChTX (light shaded) with that obtained from the last umbrella window (dark shaded). The side chains of the residues Z1′, V16′, and L20′ are explicitly shown. K27′ (in licorice representation) is also displayed to give a sense of orientation. (Dashed lines) The V16′-L20′ hydrogen bond in the last turn of the α-helix, which is broken by tidal forces during pulling. Biophysical Journal 2009 96, 2577-2588DOI: (10.1016/j.bpj.2008.12.3952) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 9 Average distances of interacting pairs in the KcsA channel and ChTX, plotted as a function of the reaction coordinate z. Additional pair distances are included in the K27′ plot to show its sequential transfer along the channel backbone. The trajectory data are from the k-20 umbrella sampling simulations. Error bars indicate one standard deviation. Biophysical Journal 2009 96, 2577-2588DOI: (10.1016/j.bpj.2008.12.3952) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 10 Orientation and fluctuations of the dipole moment of ChTX plotted as a function of the reaction coordinate z. The angle θ is defined between the dipole moment and the −z axis (toward the channel). (Inset) Polar graph of the dipole moment sampled from all the k-20 umbrella windows, where individual data points are plotted as a vector with angle θ from the channel axis and radius equal to its dipole magnitude. Error bars indicate one standard deviation. Biophysical Journal 2009 96, 2577-2588DOI: (10.1016/j.bpj.2008.12.3952) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 11 Number of water molecules in the KcsA channel-ChTX interface plotted as a function of the reaction coordinate z. (Dashed line) Relevant PMF values, purely for comparison purposes. Trajectory data are derived from the k-20 umbrella sampling simulations. Biophysical Journal 2009 96, 2577-2588DOI: (10.1016/j.bpj.2008.12.3952) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 12 PMF estimate for the conversion of the ChTX structure from the NMR conformer to the distorted conformer. The horizontal axis refers to the COM distance between V16′ backbone and L20′ backbone. Individual work functions are shown in shading, while the PMF obtained from Jarzynski's equation is shown in solid representation. Biophysical Journal 2009 96, 2577-2588DOI: (10.1016/j.bpj.2008.12.3952) Copyright © 2009 Biophysical Society Terms and Conditions