Visualizing Gas Permeation Pathways Through Proteins at ......2012/09/06 · Y. Wang, S. Shaikh,...
Transcript of Visualizing Gas Permeation Pathways Through Proteins at ......2012/09/06 · Y. Wang, S. Shaikh,...
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Emad TajkhorshidComputational Structural Biology and Molecular Biophysics
www.csbmb.beckman.illinois.edu
Department of BiochemistryCenter for Biophysics and Computational Biology
Beckman Institute for Advanced Science and TechnologyUniversity of Illinois at Urbana-Champaign
Visualizing Gas Permeation Pathways Through Proteins at Sub-Angstrom Resolution
CO2
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Solving the Newtonian equations of motion for all particles at every time step
Major limitations:
§ Time scale / sampling
§ Force field approximations
Major advantages:
§ Providing a dynamical description
§ Unparalleled spatial and temporal resolutions, simultaneously
SPEEDLIMIT
1 fs
Molecular Dynamics Simulations
nobelprize.org/nobel_prizes/chemistry/laureates/2003/animations.html
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In situ Molecular Dynamics Simulations
Atom count: 100-500k~10 ns/day on 128-1024 processors100-500 ns for each system
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Fast Growth of Computational PowerHP 735 cluster12 processors
(1993)
SGI Origin 2000128 processors (1997)
PSC LeMieux AlphaServer SC3000 processors (2002)
Ranger/Kraken ~60,000 processors (2007)
Blue Waters (UIUC) 200,000+ processors (2013)
?Anton/DESHAW/PSC512 processors (2010)
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Capturing Biology at sub-Å Resolution
5 ns
200 ns
75 ns
20 ns
100 ns
100 ns
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Large-‐Scale Transi/on of an ABC Transporter in the Membrane
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IFçèOF transi/on in an MFS Transporter in Membrane
Number of water molecules(averaged over a 1 ns window)
IF
OF
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Chemomechanical Coupling in GlpT
• IF-‐OF transi/on requires rearrangement of periplasmic salt bridges.
• Substrate affects these salt bridges.• Less work is required to induce the transi/on when the substrate is bound.
apo state
Pi-‐bound state
apo state
Pi-‐bound stat
e
IF OF
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Explicit Ligand Sampling of Gas Transport
Y. Wang, J. Cohen, W. Boron, K. Schulten, and E. Tajkhorshid, J. Struct. Biol., 2007.Y. Wang, S. Shaikh, and E. Tajkhorshid, Physiology, 2010.
POPE 100%
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Explicit Ligand Sampling of Gas Transport
Y. Wang, J. Cohen, W. Boron, K. Schulten, and E. Tajkhorshid, J. Struct. Biol., 2007.Y. Wang, S. Shaikh, and E. Tajkhorshid, Physiology, 2010.
POPE 100%
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Lipid/Water Partition Coefficients
CO2 in POPE 3.50
CO2 in POPC 2.74
O2(P) in POPC 4.04
O2(N) in POPC 3.46
O2(P) in POPE 4.73
O2(N) in POPE 5.79
ExperimentCO2 Octanol: 1.3 Hexadecane: 1.5 Olive oil: 1.7O2 Liposome: 3.9
Simulation
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Gas Diffusion Inside the Lipid Bilayer
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Gas Diffusion Inside the Lipid Bilayer
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Aquporin Water/Gas Channels
Why Tetramers?
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Implicit Ligand Sampling
Cohen, et al., 2006; Wang, et al., 2007
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Oxido-reductase and Proton Pump
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Rapid O2 Permeation via the Hydrophobic Channel in Cytochrome C Oxidase
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O2 Pathway in Cytochrome C Oxidase
Implicit ligand sampling Explicit O2 simulation
Luna VM, Chen Y., Fee JA and Stout CD (2008) Biochemistry, 47, 4657-4665 (PDB entry 3BVD)
Luna VM, Fee JA, Deniz AA and Stout CD (2012) Biochemistry, 51, 4669-4676
Observed Xenon binding in CcO ba3 crystal structures
All located along the hydrophobic channel
Reddish solid: ΔΔG map of ~ -3.5 kcal/mol ; Reddish wireframe: ΔΔG map of ~ -3.0 kcal/mol
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Simulating Membrane Gas Transport
Identical total areas
Calculating permeation rate in MD simulations
AQP1 AQP4CO2 O2 NO
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Gas Transport through Aquaporins
Typical permeation events (300-400 ps)
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Gas Occupancy/Permeation Radial Distribution
R
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A Role for the Central Pore!
Central Pore
CO2
O2
Water Pores
CO2
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Gas Transport through Aquaporins
SYSTEM TOTAL (100x100 A2) WATER PORES (4) CENTRAL PORE (1) Equi POPE-CO2 3 N/A N/A Equi POPC-CO2 5 N/A N/A Equi POPC-O2(P) 16 N/A N/A Equi POPE-O2(P) 11 N/A N/A Press POPE-CO2 168 N/A N/A Press POPC-CO2 160 N/A N/A Press POPE-O2(P) 310 N/A N/A Press POPC-O2(P) 208 N/A N/A Press POPE-AQP1-CO2 76 6 4 Press POPE-AQP1-O2(P) 79 1 6
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Free Energy Profiles for O2 and CO2
Y. Wang, J. Cohen, W. Boron, K. Schulten, and E. Tajkhorshid, J. Struct. Biol., 2007.Y. Wang, S. Shaikh, and E. Tajkhorshid, Physiology, 2010.
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Major Barrier Generated by Structured Water
Barrier identified and characterized through combining the implicit and explicit approaches
Y. Wang, J. Cohen, W. Boron, K. Schulten, and E. Tajkhorshid, J. Struct. Biol., 2007.Y. Wang, S. Shaikh, and E. Tajkhorshid, Physiology, 2010.
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NO• Permeation Through AQP4
Y. Wang, and E. Tajkhorshid, Proteins, 2010.
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NO• Permeation Through AQP4
50 ns equilibrium simulation
--- Umbrella sampling--- Implicit sampling
Y. Wang, and E. Tajkhorshid, Proteins, 2010.
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Comparison of the Central Pore in AQP1 and AQP4
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Gas Transport through Aquaporins
✦ Computational evidence for gas transport through a membrane channel
✦ Central Pore in AQPs is an optimal pathway for gas diffusion
Shared by other oligomeric membrane proteins?
✦ AQPs can be physiologically relevant gas channels in lipid bilayer with low gas permeability
✦ We can simulate very efficiently the process of gas diffusion, but we rely heavily on reliable initial configurations of lipids/protein
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Free Energy of O2 Permeation Across Charged Lipid Bilayers
DOPS / Na+
DOPS/Ca2+
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Liquid phase (30 ns) Gel phase (30 ns)
Lipid Phase and Gas Permeation
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Lipid Phase and Gas Permeation
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Highly Mobile Membrane Mimetic (HMMM) Model for Membrane Proteins and Phenomena
Ohkubo, Pogorelov, Arcario, Christensen, Tajkhorshid, Biophysical J. May 2012.
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MD Simulation with Full Membrane Representation
Collectively more than 150 ns of biased simulations
capturing a single binding event.
Z. Ohkubo and E. Tajkhorshid, Structure 2008
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Tails replaced by
organic solvent
Full model HMMM model Preserved
Replaced
DOPS
DVPS
HMMM modelHighly Mobile Membrane Mimetic model
Advantages
Increased mobility of lipids
Retain explicit headgroups allowing for atomic details
Mark Arcario
Zenmei Ohkubo
Taras Pogorelov
Josh Vermaas
Javier Baylon
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60 x 60 x 120 ÅDVPSs at 3 x 3 x 6 grid points
(22 ns)
Spontaneous and Rapid Formation of a Bilayer
Zenmei Ohkubo
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Perfect match in the membrane profile particularly in the head group region
Critical for proper description of lipid protein interactions
HMMM- Preserving the “Face” of the Lipid Bilayer
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HMMM – lipids are more mobile than full-lipids
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Spontaneous Insertion of FVII-GLA
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Spontaneous Membrane Binding (n = 10)
HMMM
HMMM Membrane
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12 ns
Spontaneous Insertion of Transmembrane Helices
t = 0
50 x 50 x 75 ÅGlycophorin A monomers: 2
z-constraint on 2 carbonyl carbons
Taras Pogorelov
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Quantitative Characterization and Optimization of HMMM
Membrane Dipolar Potential Full Membrane
HMMM
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Quantitative Characterization and Optimization of HMMMPMF of Amino Acid Insertion
Alanine
Solvent optimization
* Black lines: Full membrane data from Biophys. J. 94, 3393, 2008.
Arginine
Aspartate
Isoleucine
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Tail-Gro - Stepwise transformation of HMMMto full membrane representation
Grow tails
Full membrane
Step-wise insertion of P-glycoprotein
HMMM
Josh Vermaas
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Highly Mobile Membrane Mimetic Model (HMMM)
Shorten tails
Add solventorganic phase
Facilitating dynamical studies of membrane-associated
phenomena
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Computational Structural Biology and Molecular Biophysics Group (CSBMB)
csbmb.beckman.illinois.edu
Anton
Transporter TeamZhijian Huang Saher ShaikhJing Li Paween MahinGiray Enkavi Po-Chao WenMahmoud Moradi Wenxun GanWei Han
HMMM Team Zenmei Ohkubo Taras PogorelovMark Arcario Javier BaylonJoshua Vermaas
Collaborators:- Walter Boron - Raif Musa-Aziz- Xue Qin
- Robert Gennis
Yi Wang
Saher Shaikh
R01-GM086749 U54-GM087519R01-GM101048 P41-GM104601