Multiscale Structural Mechanics of Viruses: Stretching the ... · Multiscale Structural Mechanics...
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Multiscale Structural Mechanics of Viruses:Stretching the Limits of Continuum Modeling
William S. Klug
Mechanical & Aerospace Engineering Department
Acknowledgements:
Melissa Gibbons, Lin Ma,Chuck Knobler, Robijn Bruinsma
UCLA
Gijs Wuite, Irena Ivanovska, Wouter RoosVrije Universiteit, Amsterdam
Christoph SchmidtGeorg-August Univerität, Göttingen
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Virus Mechanics in Biology and Materials DesignEvilevitch, et al. (2003)
Packaged genomecreates forces/pressure
Protein interactions:assembly and stability
Virus-based synthetic materials(batteries, liquid crystals, solar
cells, fuel cells)
A. Belcher, MIT
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Baker, et al. (2000)
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Icosahedral Capsid Structure
CCMV
Speir, et al.
• Capsids self-assemble frommultiple copies of similaror identical proteinsubunits
http://en.wikipedia.org/wiki/Icosahedron
3
2 5
5
2 3
52 3
5
2 3
• Spherical capsids assemble with2-, 3-, & 5-fold symmetries of anicosahedron
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The Caspar-Klug Construction
Nguyen, et al.
• Form a closed shell byaligning an icosahedrontemplate onto a hexahedralsheet of “capsomers”
• Triangulation number:
(3,1) T=7
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Cowpea Chlorotic Mottle Virus (CCMV)
Speir, et al.(1995)
• T=3 Capsid assembles from 180 copies of the sameprotein subunit with 2-, 3-, & 5-fold symmetries
5
2 3
52 3
5
2 3 Johnson & Speir (1997)
• Complex “structural” phase diagram
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pH = 5native CCMV
d = 28 nm
pH = 7.5swollen CCMVexpands by 10%
Pores 2 nm in size
Structural phase transition:pH-induced conformational change
Bancroft, Hills, Markham, Virology (1967)Liu, et al., J. Struc. Biol. (2003)
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AFM: a probe for capsid mechanics
minute virus of mice (MVM)Carrasco, et al. (2006)
murine leukemia virus Kol, et al. (2006)
ϕ29Ivanovska, et al. (2004)
cowpea chlorotic mottle virus (CCMV)Michel, et al. (2006) (pH 5)Klug, et al. (2006) (pH 6)
Fundamental revelations:
Can sustain nanoNewton-sized forces
Deform elastically (reversibly)up to 5-70% of initial height
Large linear regime in elasticresponse
Excessive force usually leadsto failure/breakage
Properties affected by
• presence of genome,orientation, pH, proteinmutations, maturation
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AFM nanoindentation of CCMV at varied pH
Observations:
• Capsids are linearly elastic even at ratherlarge deformation
• Stiff and brittle at pH 5,
• 3 times softer and perfectly elastic at pH 6
• No apparent difference in structure
Can we account for these features withmodeling and simulation?
pH 6
pH 5
~3.5 nm
~20 nm
Michel, et al., PNAS, (2006)Klug, et al., PRL, (2006)
J.-P. Michel, C. Knobler (UCLA)I. Ivanovska, G. Wuite, C. Schmidt, (Vrije Universiteit Amsterdam)
Loading
Unloading
Z Indentation
Z
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Questions for theoryand simulation:
• Why is capsid force response linear for such largeindentations?
• Why do some capsids fail and others not? (Geometric?Constitutive?)
• How do local protein structure and conformationalchanges affect the global mechanical response of theshell?
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Strategy: coarse-grained Modeling
• Systematically throw away as many DOF aspossible while keeping the essential physics
Push the limits of continuum modeling
Multi-scale simulation
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Simple Continuum Model: Spherical ShellAfter all, aren’t capsids more spherical than cows?
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The Finite Element Method (FEM)
Quarter capsid w/symmetry boundary
conditions
Rigid sphericalindentor
Rigid plate
• Discretize shape into mesh of simple polyhedralelements (tetrahedra, hexahedra,etc.)
• Approximate displacements locally on elementdomains by interpolation simple polynomialbasis functions
• Minimize energy with respect to nodal fieldvalues (Ritz Method)
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Spherical CCMVSimulate indentation using different constitutive laws
• Parameterize Young’s modulus to fit experiment: E = 280 MPa• Indentation response insensitive to constitutive law.• Proper treatment of finite deformations and rotations is crucial!
Gibbons & Klug, PRE (2007)
• Hookean:
• Neo-Hookean and Mooney-Rivlin:(Nonlinear rubber elasticity)
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Spherical CCMVVarying shell thickness
• Thicker shells show Hertzianstiffening nonlinearity
• Thinner shells show softeningnonlinearity
• Almost perfectly linear for nominalCCMV thickness t = 3 nm
Key Lessons:• Shell response insensitive to constitutive law.• Linearity of force-indentation curve explained with shell mechanics.• Geometry more important than constitutive behavior.
Gibbons & Klug, PRE (2007)
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Questions for theoryand simulation:
• Why is capsid force response linear for such largeindentations?
• Why do some capsids fail and others not? (Geometric?Constitutive?)
• How do local protein structure and conformationalchanges affect the global mechanical response of theshell?
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Buckling of elastic shells with disclinations• 2-D Föppl-von Kármán shell model
• Add/remove a slice from hexagonalsheet → stretching needed to keep itflat. Buckling may alleviate stretching.
• Stabilitiy of planar sheet controlled byFöppl-von Kármán number:
• Buckled disclinations implicated indetermining the “facetedness” ofcapsids
Seung & Nelson, Phys. Rev. A (1988)
2-D Young’smodulus
bendingmodulus
5-fold disclination
Lidmar, Mirny, & Nelson, Phys. Rev. E (2003)
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Baker, et al. (2000)
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Can AFM indentation trigger buckling?
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pH-sensitivity of CCMV andchanging FvK number?
pH 6
pH 5
Klug, et al., Phys. Rev. Lett., 97, 228101 (2006)
• Explain change in stiffness as change inmaterial properties.
• Stretching modulus Y affects slope andstability
F! "Y#
R
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pH = 5native CCMV
d = 28 nm
pH = 7.5swollen CCMVexpands by 10%
How does swelling transition affectmechanical response?
pH 6
pH 5
?
Note: capsids appear structurally identicalat pH 5 and 6, and differ only in mechanicalresponse.
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Amplitude and direction of motion (a) structural data (b) normal mode 24
Tama and Brooks, J. Mol. Bio. (2002)
Normal-mode Analysis of pH-InducedSwelling of CCMV
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Ginzburg-Landau theory of swelling transitionas a structural phase transition
Klug, et al., Phys. Rev. Lett. (2006)Guérin & Bruinsma, Phys. Rev. E (2007)
Order parameter: = amplitude of soft swelling mode
Free energy:
Linearizing with respect to order parameter:
• Increasing pH softens welling mode and reduces effectiveYoung’s Modulus Y* and (to lowest order) does not affect κ.
• pH 5 failure may be initiated by buckling (geometric failure).
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Maturation of Bacteriophage HK97• Translations and rotations of the subunits (conformational
change) make the final stable mature capsid possible
Chainmail in HII
Different phases during HK97 maturation (Wikoff et. al. 2006) HK97
Cross section of PII, R~24 nm
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Parameters for HK97
Simulated result
Experimental structures
Two equilibrium configurations.Both are stable.
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Phase Transition Triggered byIndentation
Model Predictions:• Contraction transition not reversed upon unloading.• Considerable hysteresis.• Experiments in progress…
Jump from swollen tocontracted
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Questions for theoryand simulation:
• Why is capsid force response linear for such largeindentations?
• Why do some capsids fail and others not? (Geometric?Constitutive?)
• How do local protein structure and conformationalchanges affect the global mechanical response of theshell?
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CCMV (native and swollen)
HK97 (procapsid and mature) Hepatitis B
ϕ29
• Model capsid as homogeneous elastic shell (geometricheterogeneity only, for now)
• Obtain geometry from structural biology data: X-ray crystallography
→ all atom coordinates (RCSB Protein Data Bank) Cryo-electron microscopy
→ electron density maps (Electron Microscopy Data Bank)
• Triangulate molecular surfaces
• Build 3-D meshes of interior(tetrahedra fill in space between inner and outer surfaces)
Nonuniform Finite Element Models
Gibbons and Klug, Biophys J, 95(8), October 15, 2008.
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Tetrahedral Finite-Element Meshes of CCMV
Native (pH 5) Swollen (pH 7)
• Meshes given same mass and constitutive properties(hyperelastic with E=215MPa)
• 10x fewer nodes than atoms
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Indentation Simulations
• Same mass and constitutive properties (E=215MPa)• Local changes in geometry affect response:
Swollen roughly twice as soft as native Swollen more nonlinear than native
SwollenNative
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ContactFroces (pN)
Softening from bending“arms” between capsomers
Contact formed withmultiple capsomers
Buckling event
• Model Predictions: Orientation-dependent nonlinearities 3-, 5-fold: softening from local
deformation mode (arm bending) 2-fold: Buckling at high indentation
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Conclusions andUnanswered Questions
• Coarse-grained finite element modeling:→ local heterogenieties affect global mechanical response
Shell geometry key to global response 5-fold disclinations focus stress and may facilitate failure Single-protein conformational change Nonuniform capsid topography
• Test predictions via indentation experiments on pH 7 CCMVand HK97 (in progress with Wuite and Schmidt).
• 3-D model of pH 5 capsid doesn’t buckle - is failureactually consitutitve (e.g., fracture/bond-breaking)?
• How important is constitutive heterogeneity? (Need info from atomic interactions)
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Constitutive Heterogeneity:FEM + rigidity percolation
(Ongoing work with M. Thorpe, ASU)
• Compute flexibility map withconstraint theory using FIRSTsoftware
• Assign local elastic moduli to FEmodel based on flexibility map
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Constitutive Heterogeneity:Steering MD with FEM
(Ongoing work with P. Freddolino, A. Arkhipov, & K. Schulten, UIUC)
1. Steer atoms according to FE interpolation
2. MD relaxation
3. Project atomic forces onto FE nodes
4. Time or descent step with FE nodal DOF
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Thanks for your attention