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A Viscoelastic Model to Explore Force Mechanotransduction within the Focal Adhesion Complex

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Title: A Viscoelastic Model to Explore Force Mechanotransduction within the Focal Adhesion Complex


1
A Viscoelastic Model to Explore Force
Mechanotransduction within the Focal Adhesion
Complex
  • Ricardo R. Brau
  • Nicholas A. Marcantonio
  • BE. 400 Project
  • December 11, 2002

2
Overview
  • Motivation
  • Mathematical Model
  • Model Results
  • Proposed Experiments
  • Conclusion

3
Motivation Signal Transduction or Transmission
  • External forces Important in Development
    ?induction of biological responses in cells
    (apoptosis, differentiation, etc.)
  • Interface between mechanics and biochemistry must
    be explored
  • Localized Model vs. Decentralized Model for
    Mechanotransduction
  • Want to use model to examine localization of
    deformation in FAC
  • Explore potential for signal transduction due to
    molecular deformation in FAC vs. cytoskeleton

Krammer et al, 1999 Shafrir and Forgacs, 2001
Bao, 2002
4
Deformations of Single Molecules
  • Most experimentation performed on rodlike
    molecules (DNA/RNA and titin), molecular motors
    (kinesin and myosin), and fibronectin

Kellermayer et al, 1999
5
The Focal Adhesion Site
Zamir and Geiger, 2001
6
Model System
Applied Force
  • FAC is highly dynamic, and not well characterized
  • Want to start with simple model

Membrane
ß
a
aalpha ?beta Ppaxillin Ttalin Vvinculin Aact
in
P
T
V
A
Zamir and Geiger, 2001
7
Mechanical Deformations in Biology
  • Assume m0
  • ? controls kinetics
  • k affects steady-state and kinetics
  • Model molecules as viscoelastic elements

Bao, 2002
8
Model Assumptions
  • Deformation, not relative molecular position,
    determines signaling
  • Relative deformation ?x
  • Strain ?x/L
  • FAC structure is time-invariant
  • Signaling due to molecular deformation, not
    disruptions in FAC structure
  • 2o and 3o structures preserved
  • hinge motion between molecules not significant
  • Molecules can be represented as single domains

Subbiah, 1996 Oberhauser et al, 1998 Idiris et
al, 2000
9
Viscoelastic Model of the FAC
10
Mathematical Model
  • 6 unknowns and 6 equations

(1) (2) (3) (4) (5) (6)
11
Mathematical Model
  • Solve numerically using MATLAB ode23s
  • Initial condition system is at rest

FForcing Matrix SSpring Matrix DDamping
Matrix
12
Parameter Estimation
  • Molecular breathing due to thermal forces 1pN
  • Domain unfolding 100 pN
  • Deformation length scales 0.05-5 nm
  • Deformation time scales 10 nsec
  • Only actin well characterized as mechanical
    element
  • Only molecular weight information available for
    other molecules

Marszalek et al, 1999 Zhu et al, 2000 Craig et
al, 2001 Bao, 2002
13
Parameter Estimation
  • Hydrodynamic radius model molecules as spheres
  • Since ? only affects kinetics, assume similar for
    all molecules 60 pN sec/m
  • k .02 nN/nm for 172 kDa molecule, consider
    proportional to molecular weight
  • Signaling occurs at arbitrary threshold of 10
    strain

Fisher et al, 1999 Bao, 2002,
14
Parameter Estimation
  • Scenario 1
  • Each protein has same spring constant
  • Length is calculated as a function of MW
    (hydrodynamic radius)
  • Measure strain (?x/L)
  • ?x will be the same for each protein, but strain
    will be different
  • Scenario 2
  • Each protein has the same length
  • k is proportional to MW
  • Based on k.02 N/m for MW of 172 kDa
  • Measure strain (?x/L)
  • L will be the same for each protein, but ?x will
    be different
  • Perform simulations for static and dynamic loading

15
Model Results
  • Static Force 4 pN (thermal force)

16
Model Results (cont.)
17
Model Results (cont.)
18
Model Results (cont.)
19
Model Results (cont.)
20
Experimentation/Model Validation
  • Determine crystal structures and binding sites of
    FAC molecules
  • Determine mechanical properties of molecules of
    interest
  • AFM
  • Optical Tweezers
  • Single Molecule Fluorescence

Mehta et al., 1999 Lang et al., 2002
21
Experimentation/Model Validation
  • Recreate FAC in vitro (within microfluidic
    chambers) and subject to external loadings
  • Extend model to analyze kinetically varying FAC
  • Analyze FAC from a finite elements perspective,
    taking into account individual domain linkages,
    deformations, and unfolding

22
Experimentation/Model Validation
  • Study effects of mechanical deformations on
    catalytical activities of enzymes and proteins
    present in FAC

Catalysis rate function of deformation kk(?x)
Enzyme
23
Model Analysis
  • Loading dependent response
  • Static loading
  • Dynamic loading
  • Complex transient response
  • Identification of resonant frequency
  • Deformation of proteins dictated by their
    mechanical properties
  • Suggests that mechanochemical coupling occurs at
    FAC
  • Supports localized signaling

24
Conclusions
  • Model needs to be complemented by experimental
    data
  • Results provide insight into protein synthesis of
    dynamically loaded cells in culture
  • Deformations predicted by model correlate well
    with single molecule simulations and experimental
    data
  • Does not rule out energy propagation
    as described by tensegrity and
    percolation models

Shafrir and Forgacs, 2001
25
Acknowledgements
  • Ali Khademhosseini
  • Doug Lauffenburger
  • Paul Matsudaira
  • BE.400 Class

26
References
  • Ali MH, Shumaker PT (2002) Endothelial responses
    to mechanical stress where is the mechanosensor.
    Crit Care Med 30S198-206.
  • Bao G (2002) Mechanics of biomolecules. J Mechs
    Phys Solids 502237-74.
  • Craig D, Krammer A, Schulten K, and Vogel V
    (2001) Comparison of the early stages of forced
    unfolding for fibronectin type III modeuls. Proc
    Natl Acad Sci 98(10)5590-5.
  • Idris A, Alam MT, and Ikai A (2000) Spring
    mechanics of alpha-helical peptides. Protein Eng
    13763-70.
  • Fisher TE, Marszalek PE, Oberhauser AF,
    Carrio-Vazquez M, and Fernandez JM (1999) The
    micro-mechanics of single molecules studied with
    force microscopy. J Physiol 502(1)5-14.
  • Kellermayer MSZ, Smith SB, Granzier HL, and
    Bustamante C (1999) Folding-unfolding transitions
    in single titin molecules characterized with
    laser tweezers. Science 2761112-6.
  • Lang et al. (2002) Personal communication.
  • Marszalek PE, Lu H, Li H, Carrion-Vazquez M,
    Oberhauser AF, Schulten K, and Fernandez JM
    (1999) Mechanical unfolding intermediates in
    titin molecules. Nature 402100-3.
  • Mehta AD, Rief M, Spudich JA, Smith DA, and
    Simmons RM (1999) Single-molecule biomechanics
    with optical methods. Science 2831689-95.
  • Oberhauser AF, Marszalek PE, Erickson HP,
    Fernandez JM (1998) The molecular elasticity of
    the extracellular matrix protein tenascin. Nature
    393181-5.
  • Shafrir Y and Forgacs G (2001) Mechanotransduction
    through the cytoskeleton. Am J Physiol Cell
    Physiol 282C479-86.
  • Subbiah S (1996) Protein Motions. Chapman Hall,
    Austin, TX.
  • Zamir E and Geiger B (2001) Components of
    cell-matrix adhesions. J Cell Sci 1143577-9.
  • Zamir E and Geiger B (2001) Molecular complexity
    and dynamics of cell-matrix adhesions. J Cell Sci
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  • Zhu C, Bao G, and Wang N (2000) Cell mechanics
    mechanical response, cell adhesion, and molecular
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