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.

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

Introduction to Protein Structures - Molecular Graphics Tool

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

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

Steered Molecular Dynamics Introduction and Examples

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

ATPase Synthase - A Molecular Double Motor

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

Structural investigation of single biomolecules

Packing of Secondary Structures

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

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

Molecular mechanisms of cellular mechanicsw

Introduction to Protein Structures - Molecular Graphics Tool

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

Mechanical Unfolding of a -Hairpin Using Molecular Dynamics

Stretching lattice models of protein folding

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

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

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

Signaling Proteins: Mechanical Force Generation by G-proteins G

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

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

Supplementary Materials for

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

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

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

Dana Alsulaibi. Jaleel G.Sweis. Mamoon Ahram

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

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

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

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

Recently developed single-molecule atomic force microscope

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

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

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

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

COMPUTER MODELING OF FORCE-INDUCED TITIN DOMAIN UNFOLDING

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

Protein Structure Basics

What binds to Hb in addition to O 2?

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

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

Secondary structure stability, beta-sheet formation & stability

Lecture 34 Protein Unfolding Thermodynamics

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

Structure Investigation of Fam20C, a Golgi Casein Kinase

Energetics and Thermodynamics

Protein structure forces, and folding

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

Secondary and sidechain structures


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

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

Protein Folding Prof. Eugene Shakhnovich

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

Cells to Tissues. Peter Takizawa Department of Cell Biology

BMB November 17, Single Molecule Biophysics (I)

Analysis of MD trajectories in GROMACS David van der Spoel

FoldingandStretchinginaGo-likeModelofTitin

SUPPLEMENTARY INFORMATION

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

Model Mélange. Physical Models of Peptides and Proteins

Ch 3: Chemistry of Life. Chemistry Water Macromolecules Enzymes

Measurements of interaction forces in (biological) model systems

The Molecular Dynamics Method

Protein Structures: Experiments and Modeling. Patrice Koehl

Central Dogma. modifications genome transcriptome proteome

Protein NMR spectroscopy

Other Cells. Hormones. Viruses. Toxins. Cell. Bacteria

SUPPLEMENTARY INFORMATION

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

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

Protein Unfolding under Force: Crack Propagation in a Network

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

The Molecular Dynamics Method

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

How the integrin head transitions to the high- affinity

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

schematic diagram; EGF binding, dimerization, phosphorylation, Grb2 binding, etc.

Lecture 10 (10/4/17) Lecture 10 (10/4/17)

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

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

From Amino Acids to Proteins - in 4 Easy Steps

VMD: Visual Molecular Dynamics. Our Microscope is Made of...

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

The four forces of nature. Intermolecular forces, surface forces & the Atomic Force Microscope (AFM) Force- and potential curves

Protein Folding. I. Characteristics of proteins. C α

ALL LECTURES IN SB Introduction

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

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 mm 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 mm 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 m 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 a Native FnIII 10 Thr 94 C a 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

Modeling Fibronectin type III 1 NMR Structure + SMD Modeling Mu Gao Collaboration with V. Vogel, David Craig, O. Lequin

Architecture of beta-sheets This protein features a particularly strong (red) beta-sheet

Constant velocity pulling stretches and breaks first the green beta-sheet, exhibits then a stable intermediate, before the red beta-sheet is stretched and broken

Energetics of FN-III-1 during stretching

Adhesion Proteins of the Immune System

Strengthening the Immune System M. Bayas and D. Leckband Infections are battled best by the human immune system when there exists a memory from a previous disease or vaccination. The first step in using this line of defense is recognition: Cells of the immune system capture antigens, e.g., microbes in the respiratory tract, then mature in the lymph system, and finally present on their surface pieces of the antigen to T-cells that may recognize the antigen and become activated. The recognition of the antigen by T-cells is dramatically enhanced through surface receptors, CD2 and CD58, on the T-cell and the antigen presenting cell. The receptors stick out from their cell, adhere to one another, and conjoin the T-cell and antigen presenting cell long enough to enable recognition and activation. The molecular basis of this adhesion has been probed in a recent collaborative study with UIUC chemical engineer D. Leckband. Starting from the available crystallographic structure of the CD2-CD58 complex the researchers carried out 90,000 and 100,000 atom simulations using NAMD and pulled the complex apart in steered molecular dynamics simulations. An analysis of the simulations with VMD revealed in atomic level detail how the human immune system is strengthened through elastic adhesion.

CD2-CD48 interaction enhances antigen recognition between t-lymphocyte cells and antigen presenting cells CD2-CD-48: Cluster of differentiation (CD) antigen number for unique reactivity patterns with leukocytes. TCR: t cell receptor. MHC: major histocompatibility Complex. Thousands of CD s with low adhesion affinity assist cells in antigen recognition CD2-CD48 salt bridges contribute to specificity, but are they also important for the tensile strength of interaction? Yes! How do Ig domains of CD2-CD48 contribute to adhesion elasticity: through unfolding and/or deformation? Through unfolding, even though Ig domains do not contain disulfide bonds! Marcos Bayas, D. Leckband, K. Schulten, Biophys. J. 84:2223-2233, 2003

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 b 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 seperatre.