Mechanical Proteins. Stretching imunoglobulin and fibronectin. domains of the muscle protein titin. Adhesion Proteins of the Immune System

Similar documents
Mechanical Proteins. Stretching imunoglobulin and fibronectin. domains of the muscle protein titin. Adhesion Proteins of the Immune System

Steered Molecular Dynamics Studies of Titin Domains

Steered Molecular Dynamics Introduction and Examples

The Key Event in Force-Induced Unfolding of Titin s Immunoglobulin Domains

Improved Resolution of Tertiary Structure Elasticity in Muscle Protein

Don t forget to bring your MD tutorial. Potential Energy (hyper)surface

Free energy calculation from steered molecular dynamics simulations using Jarzynski s equality

Multimedia : Fibronectin and Titin unfolding simulation movies.

Steered Molecular Dynamics Introduction and Examples

Forced Dissociation of the Strand Dimer Interface between C-Cadherin Ectodomains

A structural model for force regulated integrin binding to fibronectin s RGD-synergy site

PROOF. Forced Dissociation of the Strand Dimer Interface between C-Cadherin Ectodomains. M.V. Bayas 1, K.Schulten 2 and D.

NIH Center for Macromolecular Modeling and Bioinformatics Developer of VMD and NAMD. Beckman Institute

Introduction to Protein Structures - Molecular Graphics Tool

Structural investigation of single biomolecules

ATPase Synthase - A Molecular Double Motor

Mechanical Unfolding of a -Hairpin Using Molecular Dynamics

NIH Center for Macromolecular Modeling and Bioinformatics Developer of VMD and NAMD. Beckman Institute

Stretching the Immunoglobulin 27 Domain of the Titin Protein: The Dynamic Energy Landscape

Stretching lattice models of protein folding

Molecular dynamics simulations of anti-aggregation effect of ibuprofen. Wenling E. Chang, Takako Takeda, E. Prabhu Raman, and Dmitri Klimov

Molecular mechanisms of cellular mechanicsw

Structural and mechanistic insight into the substrate. binding from the conformational dynamics in apo. and substrate-bound DapE enzyme

Supplementary Materials for

There is a growing interest in the kinetic mechanisms by which. Water s role in the force-induced unfolding of ubiquitin

Energy Landscape Distortions and the Mechanical Unfolding of Proteins

Packing of Secondary Structures

The living cell is a society of molecules: molecules assembling and cooperating bring about life!

Introduction to Protein Structures - Molecular Graphics Tool

Tertiary and Secondary Structure Elasticity of a Six-Ig Titin Chain

Thermal Effects in Stretching of Go-like Models of Titin and Secondary Structures

Non-Native Interactions Are Critical for Mechanical Strength in PKD Domains

Contour Length and Refolding Rate of a Small Protein Controlled by Engineered Disulfide Bonds

Scanning Force Microscopy. i.e. Atomic Force Microscopy. Josef A. Käs Institute for Soft Matter Physics Physics Department. Atomic Force Microscopy

Stabilization Provided by Neighboring Strands Is Critical for the Mechanical Stability of Proteins

Recently developed single-molecule atomic force microscope

COMPUTER MODELING OF FORCE-INDUCED TITIN DOMAIN UNFOLDING

Hands-on Course in Computational Structural Biology and Molecular Simulation BIOP590C/MCB590C. Course Details

Protein Dynamics. The space-filling structures of myoglobin and hemoglobin show that there are no pathways for O 2 to reach the heme iron.

Secondary Structure. Bioch/BIMS 503 Lecture 2. Structure and Function of Proteins. Further Reading. Φ, Ψ angles alone determine protein structure

Signaling Proteins: Mechanical Force Generation by G-proteins G

FACTORS IN MECHANICAL STABILITY OF PROTEIN L : A STEERED MOLECULAR DYNAMICS STUDY R. ADITAMA, R. HERTADI *

NSF Summer School UIUC 2003 Molecular Machines of the Living Cell : Photosynthetic. Unit from Light Absorption to ATP Synthesis Melih Sener

Thesis. Presented in Partial Fulfillment of the Requirements for the Degree Master of Science in the Graduate School of The Ohio State University

Secondary and sidechain structures

Outline. Levels of Protein Structure. Primary (1 ) Structure. Lecture 6:Protein Architecture II: Secondary Structure or From peptides to proteins

Retinal Proteins (Rhodopsins) Vision, Bioenergetics, Phototaxis. Bacteriorhodopsin s Photocycle. Bacteriorhodopsin s Photocycle

1. What is an ångstrom unit, and why is it used to describe molecular structures?

SUPPLEMENTARY INFORMATION

FoldingandStretchinginaGo-likeModelofTitin


Computational Structural Biology and Molecular Simulation. Introduction to VMD Molecular Visualization and Analysis

Lecture 2 and 3: Review of forces (ctd.) and elementary statistical mechanics. Contributions to protein stability

BMB November 17, Single Molecule Biophysics (I)

arxiv:q-bio/ v1 [q-bio.bm] 16 Dec 2004

Protein Folding Prof. Eugene Shakhnovich

A conserved P-loop anchor limits the structural dynamics that mediate. nucleotide dissociation in EF-Tu.

Quantification of the stiffness and strength of cadherin ectodomain binding with different ions

Lecture 34 Protein Unfolding Thermodynamics

Protein Structure Basics

Steered Molecular Dynamics Simulation of the Rieske Subunit Motion in the Cytochrome bc 1 Complex

Protein Unfolding under Force: Crack Propagation in a Network

Structure Investigation of Fam20C, a Golgi Casein Kinase

Signal Transduction Phosphorylation Protein kinases. Misfolding diseases. Protein Engineering Lysozyme variants

Secondary structure stability, beta-sheet formation & stability

Announcements. Homework 3 (Klaus Schulten s Lecture): Due Wednesday at noon. Next homework assigned. Due Wednesday March 1.

Evolution of Translation: Dynamics of Recognition in RNA:Protein Complexes

Central Dogma. modifications genome transcriptome proteome

The Molecular Dynamics Method

Many proteins spontaneously refold into native form in vitro with high fidelity and high speed.

Single Molecule Force Spectroscopy Reveals that Electrostatic Interactions Affect the Mechanical Stability of Proteins

Computer simulations of protein folding with a small number of distance restraints

Outline. Levels of Protein Structure. Primary (1 ) Structure. Lecture 6:Protein Architecture II: Secondary Structure or From peptides to proteins

letters to nature ... Reverse engineering of the giant muscle protein titin

Visualizing folding of proteins (1 3) and RNA (2) in terms of

Equilibrated atomic models of outward-facing P-glycoprotein and effect of ATP binding on structural dynamics (Supplementary Information)

Protein Structure. W. M. Grogan, Ph.D. OBJECTIVES

Part III - Bioinformatics Study of Aminoacyl trna Synthetases. VMD Multiseq Tutorial Web tools. Perth, Australia 2004 Computational Biology Workshop

Dana Alsulaibi. Jaleel G.Sweis. Mamoon Ahram

Molecular Dynamics Investigation of the ω-current in the Kv1.2 Voltage Sensor Domains

Supporting Information. for An atomistic modeling of F-actin mechanical responses and determination of. mechanical properties

PROTEIN STRUCTURE PREDICTION USING GAS PHASE MOLECULAR DYNAMICS SIMULATION: EOTAXIN-3 CYTOKINE AS A CASE STUDY

Protein Structures: Experiments and Modeling. Patrice Koehl

The Molecular Dynamics Method

Polypeptide Folding Using Monte Carlo Sampling, Concerted Rotation, and Continuum Solvation

Biochemistry,530:,, Introduc5on,to,Structural,Biology, Autumn,Quarter,2015,

Mechanical Engineering of Elastomeric Proteins: Toward Designing New Protein Building Blocks for Biomaterials**

From Amino Acids to Proteins - in 4 Easy Steps

Supporting Online Material for

Single molecule force spectroscopy reveals a highly compliant helical

Protein NMR spectroscopy

Presenter: She Zhang

Energetics and Thermodynamics

Analysis of MD trajectories in GROMACS David van der Spoel

Massachusetts Institute of Technology Harvard Medical School Brigham and Women s Hospital VA Boston Healthcare System 2.79J/3.96J/BE.

Electro-Mechanical Conductance Modulation of a Nanopore Using a Removable Gate

Elasticity and Rupture of a Multi-Domain Neural Cell Adhesion Molecule Complex

Supplementary Figures:

Proteins are not rigid structures: Protein dynamics, conformational variability, and thermodynamic stability

Govardhan Reddy. John E. Straub. D. Thirumalai*

Transcription:

Mechanical Proteins F C D B A domains of the muscle protein titin E Stretching imunoglobulin and fibronectin G NIH Resource for Macromolecular Modeling and Bioinformatics Theoretical Biophysics Group, Beckman Institute, UIUC Adhesion Proteins of the Immune System

Immunoglobulin Domains

AFM Studies of Titin And FN-III Modules AFM tip Forced unfolding of identical modules occurs one by one v Force (pn) 600 400 0 Titin I27 0 50 100 150 Force (pn) FN-III Extension (nm) Extension (nm) Reviewed in Fisher et al. Nature Struct. Biol. 7:719-724 (2001)

Contracting and Relaxing Muscle Needs ATP!

Titin the Longest Protein in the Human Genome titin I-band sarcomere 2 µm I1 PEVK region; random coil I27 I41 Under weak forces, the PEVK region extends (entropic spring) titin immunoglobulin-like (Ig) domain 40 Å Under intermediate forces, Ig domains stretch by ~10A; under strong forces, they unfold one by one, by 250A

Probing the Passive Elasticity of Muscle: I27 Marszalek et al., Nature, 402,100-103 (1999) Krammer et al., PNAS, 96, 1351-1356 (1999) Lu et al., Biophys. J., 75, 662-671 (1998) sarcomere Computational Stretching of Ig: Trajectory Animation titin immunoglobulin-like (Ig) domain Gaub et al., Fernandez et al. Hui Lu, Barry Isralewitz

Quantitative Comparison Bridging the gap between SMD and AFM experiments Steered Molecular Dynamics (SMD) Force-extension curve Force-pulling velocity relationship AFM range Current SMD range Target simulation range SMD data AFM data Extrapolation of AFM data Extension curve Hui Lu, Barry Isralewitz

Stretching modular proteins Detailed View Extension occurs in two steps extension Schematic view and typical Extension vs. force plot Distribution of measured forces For step 1 and step 2

Two Force Bearing Components Two types of SMD simulations I. Native structure (2 A of extension) II. Mechanical unfolding intermediate (10 A of extension) III. Unfolded state (250 A of extension) Constant velocity: Lu et al, Biophys J., 72, 1568 (1007) three force interstrand (A B) hydrogen bonds Hui Lu, Barry Isralewitz six interstrand (A G) hydrogen bonds Constant force: Lu and Schulten, Chem. Phys., 247 (1999) 141. Reviewed in Isralewitz et al. Curr. Opinion Struct. Biol. 11:224-230 (2001)

Water-Backbone Interactions Control Unfolding A B A' G 1000 pn 750 pn During stretching, water molecules attack repeatedly interstrand hydrogen bonds, about 100 times / ns; for forces of 750 pn water fluctuation controls unfolding! E12 water greases protein folding! Lu and Schulten, Biophys J.79: 51-65 (2000)

Titin Domain Heterogenity: Comparing Oxidized and Reduced I1 titin I 1 I 27 PEVK oxidized reduced Stretching I 1 with constant velocity titin I 1 Mayans et al. Structure 9:331-340 (2001) B A A G I 1 in 70 Å water sphere of 70 Å (18,000 atoms) F disulfide bond titin I27 Use of program NAMD on 32 Processor (1.1 GHz Athlon) Linux cluster: 1 day/ns Mu Gao

Titin Domain Heterogenity: I 1 I 27 pre-stretching slack tight in I1 Stretching with constant force of 750 pn titin I 1 Mayans et al. Structure 9:331-340 (2001) Hydrogen bond energies /(Kcal/mol) I 1 in 70 Å water sphere of 70 Å (18,000 atoms) B A A E3(H)-K31(O) G F PEVK 6 A-B bonds tight slack disulfide bond E3(O)-K31(H) time / ps titin I27 3 A-B bonds easy slack K6(H)-V29(O) Use of program NAMD on 32 Processor (1.1 GHz Athlon) Linux cluster: 1 day/ns K6(O)-V29(H) F8(H)-R27(O) E9(O)-R27(H) Mu Gao

Fibronectins

Architecture and Function of Fibronectin Modules Extracellular matrix Fibronectin FN-I FN-II FN-III 10 µm FN-III 7 FN-III 9 FN-III 8 FN-III 10 Fibronectin is a major component of extracellular matrix It consists of three types of modules: type I, type II, and type III Highly extensible A B 35 Å F G Andre Krammer V. Vogel, U. Wash.

Fibronectin Matrix in Living Cell Culture Force (pn) FN-III Extension (nm) 100 µ m Atomic force microscopy observations Ohashi et al. Proc. Natl. Acad. Sci USA 96:2153-2158 (1999) Andre Krammer V. Vogel, U. Wash.

RGD Loop of FnIII 10 Krammer et al. Proc. Natl. Acad. Sci USA 96:1351-1356 (1999) Gly 79 Asp 80 Arg 78 Val 1 C α Native FnIII 10 Thr 94 C α Extension of 13 Å Andre Krammer V. Vogel, U. Wash. F = 500 pn integrin interacting with extracellular matrix fibronectin binding with RGD loop to integrin http://www.ks.uiuc.edu

Probing Unfolding Intermediates in FN-III 10 F FnIII 10 module solvated in a water box 55 60 367 Å 3 (126,000 atoms) Steered Molecular Dynamics, periodic boundary conditions, NpT ensemble, Particle Mesh Edwald for full electrostatics NAMD on Linux cluster of 32 Athlon 1.1GHz processors: 10 days/ns Native Fibronectin III 10 Mu Gao, U. Illinois A. Krammer, D. Craig, V. Vogel, U. Wash.

Probing Unfolding Intermediates in FN-III 10 Specific stretching and unfolding pathway for constant force (500 pn) stretching: scenario with A rupturing first Complete stretching and unfolding pathway: after straightening and partial A- B separation, A,, or A+G or G rupture first

Stretching FN-III 1 : Pronounced Intermediate SMD simulations (150,000 atoms) M. Gao, D. Craig, O. Lequin, I. D. Campbell, V. Vogel, and K. Schulten. Structure and functional significance of mechanically unfolded fibronectin type III1 intermediates. Proc. Natl. Acad. Sci. USA, 100:14784 14789, 2003. AFM experiments Force (pn) 281±9 Å 204±16 Å 87±16 Å Extension (Å) NMR structure

Stretching FN-III 1 : Pronounced Intermediate SMD simulations (150,000 atoms) M. Gao, D. Craig, O. Lequin, I. D. Campbell, V. Vogel, and K. Schulten. Structure and functional significance of mechanically unfolded fibronectin type III1 intermediates. Proc. Natl. Acad. Sci. USA, 100:14784 14789, 2003. AFM experiments Force (pn) 281±9 Å 204±16 Å 87±16 Å Extension (Å) NMR structure

Stretching FN-III 1 : Pronounced Intermediate SMD simulations (150,000 atoms) M. Gao, D. Craig, O. Lequin, I. D. Campbell, V. Vogel, and K. Schulten. Structure and functional significance of mechanically unfolded fibronectin type III1 intermediates. Proc. Natl. Acad. Sci. USA, 100:14784 14789, 2003. AFM experiments Force (pn) 281±9 Å 204±16 Å 87±16 Å Extension (Å) NMR structure

Adhesion Proteins of the Immune System

Strengthening the Immune System CD2 and CD58 contain Ig domains 0.05 Å / ps slow Model Based on Crystal Structure: Wang et al. (1999) Cell, 97, 791 90,000 atoms NAMD simulation on Linux cluster 120 ps so far 1 0.05 Å / ps pulling velocity Marcos Bayas, D. Leckband, K. Schulten, submitted 1 Å / ps

Separation at 0.05 Å /ns Pulling : salt bridges important (Aralunandam et al 1993, 1994) for adhesion are broken last Marcos Bayas, D. Leckband, K. Schulten, Biophys. J. 84:2223-2233, 2003

Behavior of Non-Mechanical Proteins

Force-induced Unfolding of Other Domains C2 domain of synaptotagmin I (all sheet protein) no initial force peak much less resistance to external forces than Ig and FnIII during unfolding hydrogen bonds not required to be broken in clusters Lu and Schulten, Proteins, 35, 453-463 (1999) NIH Resource for Macromolecular Modeling and Bioinformatics Theoretical Biophysics Group, Beckman Institute, UIUC

Classification of β Sandwich Domains Class I a: strong resistance Class I b: less resistance Class I c: little resistance Lu and Schulten, Proteins, 35, 453-463 (1999) NIH Resource for Macromolecular Modeling and Bioinformatics Theoretical Biophysics Group, Beckman Institute, UIUC

Force-induced unfolding of alpha-helical protein Cytochrome C6 (all helix protein) no initial force peak much less resistance to external forces than Ig and FnIII during unfolding hydrogen bonds not required to be broken in clusters Lu and Schulten, Proteins, 35, 453-463 (1999) NIH Resource for Macromolecular Modeling and Bioinformatics Theoretical Biophysics Group, Beckman Institute, UIUC

Ubiquitin Fatemeh Araghi, Timothy Isgro, Marcos Sotomayor

Monoubiquitylation versus multi-ubiquitylation

Structure-Function Relationship Proteasome Degradation

First SMD Simulation First peak when the first beta strand is stretched out SMD simulation, with constant velocity Box of water 70x240x70 A ~81K atoms smd velocity 0.4 A/ps smd spring constant 7 kcal/mol A^2

Ubiquitin Unfolding I Force (pn) cv-0.02 Å/ps E64 Q2 S65 F4 L67 K6 L69 water N-term fixed 0 Å, 1 ps Q2 F4 extension (Å) K6 E64 S65 L67 L69 14 Å, 700ps Q2 F4 K6 E64 15 Å, 813ps S65 L67 L69 Mu Gao

Ubiquitin Unfolding II Extension (Å) cf-500pn K48 K48 fixed F45 I44 L50 H68 V70 L43 R42 R72 Q40 F45 K48 F45 H68 I44 H68 L43 V70 R42 V70 R72 Q40 R72 0 Å, 1 ps 9 Å, 60 ps L50 Time (ps) K48 L50 I44 L43 R42 Q40 17 Å, 320 ps R72 H68 V70 F45 Mu Gao K48 I44 L43 Q40 R42 L50 19 Å, 340 ps

Pulling Dimer SMD (v=0.4 A/ps k=7 kcal/mol A^2) constant P Two monomers separate.