Molecular Dynamics Study of the KcsA Potassium Channel

Slides:



Advertisements
Similar presentations
Voltage-Dependent Hydration and Conduction Properties of the Hydrophobic Pore of the Mechanosensitive Channel of Small Conductance  Steven A. Spronk,
Advertisements

Analysis and Evaluation of Channel Models: Simulations of Alamethicin
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.
Pedro R. Magalhães, Miguel Machuqueiro, António M. Baptista 
Hydroxide and Proton Migration in Aquaporins
Vishwanath Jogini, Benoît Roux  Biophysical Journal 
Ion Permeation through a Narrow Channel: Using Gramicidin to Ascertain All-Atom Molecular Dynamics Potential of Mean Force Methodology and Biomolecular.
Richard J. Law, Keith Munson, George Sachs, Felice C. Lightstone 
Molecular Dynamics Free Energy Calculations to Assess the Possibility of Water Existence in Protein Nonpolar Cavities  Masataka Oikawa, Yoshiteru Yonetani 
Urs Zimmerli, Petros Koumoutsakos  Biophysical Journal 
Influence of Chain Length and Unsaturation on Sphingomyelin Bilayers
Jing Han, Kristyna Pluhackova, Tsjerk A. Wassenaar, Rainer A. Böckmann 
R. Jay Mashl, H. Larry Scott, Shankar Subramaniam, Eric Jakobsson 
Fangqiang Zhu, Emad Tajkhorshid, Klaus Schulten  Biophysical Journal 
Volume 83, Issue 5, Pages (November 2002)
Steered Molecular Dynamics Simulations on the “Tail Helix Latch” Hypothesis in the Gelsolin Activation Process  Feng Cheng, Jianhua Shen, Xiaomin Luo,
Volume 102, Issue 6, Pages (March 2012)
Volume 85, Issue 2, Pages (August 2003)
The Influence of Amino Acid Protonation States on Molecular Dynamics Simulations of the Bacterial Porin OmpF  Sameer Varma, See-Wing Chiu, Eric Jakobsson 
Mechanism and Energetics of Charybdotoxin Unbinding from a Potassium Channel from Molecular Dynamics Simulations  Po-chia Chen, Serdar Kuyucak  Biophysical.
Liqun Zhang, Susmita Borthakur, Matthias Buck  Biophysical Journal 
Ben Corry, Serdar Kuyucak, Shin-Ho Chung  Biophysical Journal 
Tests of Continuum Theories as Models of Ion Channels. II
Christian Kappel, Ulrich Zachariae, Nicole Dölker, Helmut Grubmüller 
Coarse-Grained Peptide Modeling Using a Systematic Multiscale Approach
Ion Counting from Explicit-Solvent Simulations and 3D-RISM
Analysis and Evaluation of Channel Models: Simulations of Alamethicin
J.L. Robertson, L.G. Palmer, B. Roux  Biophysical Journal 
Yuno Lee, Philip A. Pincus, Changbong Hyeon  Biophysical Journal 
Homology Model of the GABAA Receptor Examined Using Brownian Dynamics
Analysis of the Stability of Hemoglobin S Double Strands
Ligand Binding to the Voltage-Gated Kv1
Modeling Diverse Range of Potassium Channels with Brownian Dynamics
Simone Furini, Carmen Domene  Biophysical Journal 
Tests of Continuum Theories as Models of Ion Channels. I
Shin-Ho Chung, Matthew Hoyles, Toby Allen, Serdar Kuyucak 
Marcos Sotomayor, Klaus Schulten  Biophysical Journal 
Sundeep S. Deol, Peter J. Bond, Carmen Domene, Mark S.P. Sansom 
Dissecting DNA-Histone Interactions in the Nucleosome by Molecular Dynamics Simulations of DNA Unwrapping  Ramona Ettig, Nick Kepper, Rene Stehr, Gero.
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 90, Issue 6, Pages (March 2006)
Volume 76, Issue 3, Pages (March 1999)
Molecular Dynamics Simulations of Wild-Type and Mutant Forms of the Mycobacterium tuberculosis MscL Channel  Donald E. Elmore, Dennis A. Dougherty  Biophysical.
Investigating Lipid Composition Effects on the Mechanosensitive Channel of Large Conductance (MscL) Using Molecular Dynamics Simulations  Donald E. Elmore,
Grischa R. Meyer, Justin Gullingsrud, Klaus Schulten, Boris Martinac 
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 111, Issue 1, Pages (July 2016)
Coupled Motions between Pore and Voltage-Sensor Domains: A Model for Shaker B, a Voltage-Gated Potassium Channel  Werner Treptow, Bernard Maigret, Christophe.
Open-State Models of a Potassium Channel
Ion-Induced Defect Permeation of Lipid Membranes
Karina Kubiak, Wieslaw Nowak  Biophysical Journal 
The Selectivity of K+ Ion Channels: Testing the Hypotheses
Michael Thomas, Dylan Jayatilaka, Ben Corry  Biophysical Journal 
Mechanism of Anionic Conduction across ClC
Mechanism of Interaction between the General Anesthetic Halothane and a Model Ion Channel Protein, III: Molecular Dynamics Simulation Incorporating a.
Sebastian Fritsch, Ivaylo Ivanov, Hailong Wang, Xiaolin Cheng 
Analysis of the Stability of Hemoglobin S Double Strands
Christian Kappel, Ulrich Zachariae, Nicole Dölker, Helmut Grubmüller 
Jochen Zimmer, Declan A. Doyle, J. Günter Grossmann 
Volume 78, Issue 6, Pages (June 2000)
Yinon Shafrir, Stewart R. Durell, H. Robert Guy  Biophysical Journal 
Siu Cheung Li, Matthew Hoyles, Serdar Kuyucak, Shin-Ho Chung 
Volume 94, Issue 11, Pages (June 2008)
Distribution of Halothane in a Dipalmitoylphosphatidylcholine Bilayer from Molecular Dynamics Calculations  Laure Koubi, Mounir Tarek, Michael L. Klein,
Fangqiang Zhu, Klaus Schulten  Biophysical Journal 
Volume 98, Issue 3, Pages (February 2010)
Molecular Dynamics Simulation of a Synthetic Ion Channel
David L. Bostick, Karunesh Arora, Charles L. Brooks 
Presentation transcript:

Molecular Dynamics Study of the KcsA Potassium Channel Toby W. Allen, Serdar Kuyucak, Shin-Ho Chung  Biophysical Journal  Volume 77, Issue 5, Pages 2502-2516 (November 1999) DOI: 10.1016/S0006-3495(99)77086-4 Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 1 (A) Cross-section of the model channel. Shown are the hydrophobic pore and selectivity filter protein. The solid curves outline the effective radius of the Lennard-Jones 5-3 hydrophobic pore. Double arrows indicate effective pore and reservoir diameters (taking into account van der Waals radii). Reservoirs extend outside the range of this figure to ±35Å where periodic boundaries are applied. Helix and mouth dipoles are represented by vector arrows. Solid lines of length 5Å oriented perpendicular to the channel axis at z=22Å represent the harmonic blockers that prevent water from moving behind the protein. (B) Projections of two subunits forming the selectivity filter. Carbon, nitrogen, and oxygen atoms are shown in white, gray, and black, respectively, while hydrogen atoms are not shown. Initial (r, z) coordinates of the carbonyl oxygen centers on the G1, Y, G2, V, and T residues, and of the T hydroxyl oxygen are (5.25, 22.97), (3.20, 20.38), (2.22, 17.26), (2.34, 14.68), (2.76, 10.23), and (3.11, 9.21) Å, respectively. Constrained groups of atoms are indicated with arrows. Gray and black arrows refer to endpoint constraints and interactions with the pore helix, respectively. Biophysical Journal 1999 77, 2502-2516DOI: (10.1016/S0006-3495(99)77086-4) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 2 Effect of harmonic constraints on energy. Each graph shows the dependence of the relative potassium (solid curve, filled circles) and sodium (dotted curve, open circles) energies with respect to the reservoir reference point (z=29Å), on the strength of harmonic constraints. (A) The uppermost panel displays the effect of the G1 force constant (KG1), applied to G1-N and H atoms, on the relative energies of potassium and sodium ions at z=20.4Å. The second row shows the effect of KY on the relative energies at z=20.4 and 17.3Å, the third row shows the effect of KG2 at positions z=17.3 and 14.7Å, and the fourth row shows the effect of KV on relative ion energies at z=14.7 and 10.2Å. (B) The dependence of relative potassium and sodium total system energies at z=17.3Å on the constraint strength applied to tyrosine side-chain atoms (ring carbons and hydroxyl oxygen). All error bars are one standard error of means. Biophysical Journal 1999 77, 2502-2516DOI: (10.1016/S0006-3495(99)77086-4) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 3 (A) Equilibrated structure for water-filled channel. (B) Equilibrated multiple ion system structure example. Water molecules are shown as small dark gray spheres, potassium ions as large black spheres. Diagrams have been generated with the use of RasMol v.2.6. Biophysical Journal 1999 77, 2502-2516DOI: (10.1016/S0006-3495(99)77086-4) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 4 Self-diffusion and rotational correlation: (A) Self-diffusion Dz (solid curve, filled circles) and Dxy (dotted curve, open circles). (B) First-order inverse rotational correlation time constant τ−1. A 5-Å grid has been used over the potassium channel with a single value for each reservoir. The dashed lines are the bulk reference values from Table 1. Error bars are one standard error of means. Biophysical Journal 1999 77, 2502-2516DOI: (10.1016/S0006-3495(99)77086-4) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 5 RDFs for potassium (A) and sodium (B) when an ion is held at z=20.4Å. The RDF including water oxygen atoms is plotted with a solid line whereas that for protein oxygens is plotted with a dotted line. The dashed curve is the bulk hydration RDF. The inset shows an ion-carbonyl oxygen geometry representative of the simulation. Biophysical Journal 1999 77, 2502-2516DOI: (10.1016/S0006-3495(99)77086-4) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 6 Positions of the first maxima in the hydration and protein oxygen radial distribution functions of potassium (A) and sodium (B). Solid curves (filled circles) are hydration RDFs, dotted curves (open circles) are protein oxygen RDFs, and the dashed lines are bulk values. Biophysical Journal 1999 77, 2502-2516DOI: (10.1016/S0006-3495(99)77086-4) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 7 First shell coordination (hydration and protein solvation) numbers for potassium (A) and sodium (B). Dotted curves (open circles) are hydration numbers, solid curves (filled circles) are total water plus protein solvation numbers, and the dashed lines are the bulk hydration numbers. Biophysical Journal 1999 77, 2502-2516DOI: (10.1016/S0006-3495(99)77086-4) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 8 (A) The total energy of the system with respect to the extracellular reservoir is plotted against ion position z for potassium (filled circles and dashed curve) and sodium (open circles and dotted curve). A profile for potassium corrected by placing mouth dipoles is drawn as a solid curve. All values are derived from simulations using the ST2 water model. Error bars are one standard error of means. (B) Potassium energy well depth (average of relative energies at points z=5 and 7.5Å) is plotted against pore helix charge. The fitted solid curve is the quadratic function E(kT)=−37+150q−295q2 with helix charge q in units 10−19 C. Biophysical Journal 1999 77, 2502-2516DOI: (10.1016/S0006-3495(99)77086-4) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 9 Energy profiles with the SPC/E water model. (A) The total energy profiles, with respect to the reservoir reference point (z=29Å) for potassium (filled circles and solid curve) and sodium (open circles and dotted curve). (B) Comparison of free and total system energy difference profiles. The difference in the free energy change, corresponding to the transformation K→Na, between each point in this profile and the reservoir reference point (z=29Å) is drawn as a solid curve (filled circles). The total system energy differences relative to the reservoir are drawn as a dotted curve (open circles). Error bars are one standard error of means. Biophysical Journal 1999 77, 2502-2516DOI: (10.1016/S0006-3495(99)77086-4) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 10 Ion trajectories. An external field of 5mV/Å2 drives ions from extracellular to intracellular. Reservoir ions are not shown. Initial z-coordinates are 18.8, 21.7, and 23.0Å. Biophysical Journal 1999 77, 2502-2516DOI: (10.1016/S0006-3495(99)77086-4) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 11 Potassium ion diffusion. Dz (solid curve) and Dxy (dotted curve) are compared to the bulk value (dashed line). Error bars are one standard error of means. Biophysical Journal 1999 77, 2502-2516DOI: (10.1016/S0006-3495(99)77086-4) Copyright © 1999 The Biophysical Society Terms and Conditions