Structure-mechanics relationship in fibrous biomaterials Mohd Suhail Rizvi and Sovan Lal Das Pravartana 2016 12th February 2016 1 Fibrous materials Articular cartilage Aorta Cellulose fibers Connective tissue Elastic fibers Collagen fibers Fibers in natural systems Engineering fibrous materials Fibrin fibers Collagen fibers Synthetic polymeric fibers Plants Applications • Scaffolds in tissue engineering • Drug delivery carriers • Filteration media and nanosensors • Wound dressing • Cosmetic skin masks 1. Anatomy 215 Virtual Microscopy, Indiana University 2. http://histologistics.com 1. Lisi et al., 2012, PLoS ONE Cells on substrates Mechanical properties of the substrates influence • Cell lineage specification1 • Cell proliferation2 and migration5 • Cytoskeletal organization3 • Cell spreading and stress fiber formation4 • Cell polarization and elongation6 Structural properties of the substrates influence • Cell morphology7 Random fibers 7,8 • Cell alignment • Cell differentiation9 • Cell migration10 • Anisotropic cell spreading11 A.J. et al., 2006, Cell et al, 2009, J. Tissue Eng. Regen. Med. 3Ghosh, K. et al., 2007, Biomaterials 4Yeung, T. et al., 2005, Cell Mot. and Cytoskel. 5Lo, C.M. et al, 2000, Biophys. J. 6Prager-Khoutorsky, M. et al., 2011, Nat. Cell Biol. 1Engler, 2Hadjipanayi, E. Aligned fibers 7Aubin, H. et al., 2010, Biomaterials S.T. et al, 2014, Biomech. Model. Mechanobiol. 9Lu, D. et al. et al., 2014, Biomaterials 10Teixeira, A.I. et al., 2003, J. Cell Sci. 11Saez, A. et al, 2007, Proc. Nat. Acad. Sci. 8Wong, 3 Existing Constitutive Models • Fibers are considered to be embedded in an isotropic substrate- fibrous composite m Energy in terms of invariants of matrix deformation Response of fiber Response of fibrous composite Limitations: • Applicable to fibrous composites with straight fibers only Holzapfel, G.A. et al., 2000, J. Elasticity Federico, S. et al., 2010, J. Royal Soc. Interface 4 Assumptions • Fibrous matrix is considered to be planar • All the fibers are of same diameter • Fiber diameter is very small (~1μm) • Fiber bending stiffness is negligible in comparison to the stretching. • Fibers fused with each other do not detach Description of fiber structure θ R l Normalized fiber length Description of matrix structure Fiber length Fiber orientation Fiber fusion (i) Fiberfiber fusion r (ii) 5 Effective fiber response • Effective fiber response is defined as the average response of the fibers passing through two points. 1 λ Fiber elongation and bending are measured in terms of changes in fiber length and fiber curvature, respectively. • The fiber curvature information is not known. 6 Fiber bending Approximation of fiber shape R l Root-mean-square (RMS) curvature of undeformed fiber RMS curvature of deformed fiber Bending energy of a fiber • Fiber curvature is approximated in terms of the fiber length • Fiber response demonstrates strain softening for compression strain stiffening for elongation 7 Effective fiber response • For curved fibers the fiber response is bending dominated Higher fiber curvature leads to soft fiber response 8 Response of the fibrous matrix x r+x r χ χ(r) χ(r+x) 9 Model validation Matrix elongation 1Experiment log Tensile modulus Change in area Shear modulus log 2Experiment • Model demonstrates qualitative agreement with the experiments. • Fiber fusion leads to stiffer matrix response • Aligned fibrous matrix has higher tensile modulus • Random fibrous matrix has higher shear modulus 1Kumar, 2Kabla, P., 2010, M. Tech. Thesis, IIT Kanpur A. et al., 2007, J. R. Soc. Interface 10 Fiber alignment • The degree of fiber alignment in the fibrous matrix can be defined as where μθ is the mean fiber orientation. • Matrix deformation leads to change in • The probability density function in the deformed configuration is where Cell-matrix interaction Fiber alignment Displacement field Our model Our model Discrete fiber model Experiment Discrete fiber model • Displacement due to a polarized cell is highest near the cell extremities. • Cellular forces lead to remodeling of the fibers in the matrix Abhilash, A.S. et al., 2014, Biophys. J. Gjorevski, N. et al., 2012, Biophysi. J. 12 Cell-cell interaction Displacement field Low Displacement High Fiber alignment Low Alignment parameter Discrete fiber model High •Fiber remodeling is observed between two cells- formation of tracks Cell-cell interaction energy Cell-cell separation Strong interaction Low Interaction energy Weak interaction High • Cell-cell interaction depends on cell orientations and their separation Abhilash, A.S. et al., 2014, Biophys. J. 13 Generalized Model • For fibrous composites with single family of straight fibers, the energy is expressed in terms of 5 invariants. • For two family fibrous composites, energy is written in terms of 9 invariants Isotropic part Family-1 fibers Family-2 fibers Fiber-fiber interaction Holzapfel, G., Nonlinear Solid Mechanics n m Generalized Model • For fibrous composites with single family of straight fibers • For fibrous composites with multiple independent families of straight fibers • For curved fibers without fiber fusion No bending stiffness Finite bending stiffness Here u is the effective fiber response. Generalized Model • Inclusion of fiber breakage- Mullins effect • Assumption- a fiber breaks if its stretch exceeds a threshold value λb • Fiber breakage or damage criterion • In general • For fibrous matrix • These relations describe the mechanical response of the fibrous composite including • Effect of curved fibers • Diverse fiber orientations • Fiber breakage Future directions • Validation of model predictions using experiments Improvement in the model • Incorporation of structural details in the model • Study of matrix response against biaxial loading • Implementation of the fibrous composite model • Microscopic mechanical response of matrix against dynamic loading Study of cell-matrix interactions • Incorporation of detailed cell geometry • Study of the fibrous matrix response against forces applied by multiple cells • Incorporation of cytoskeletal remodeling in response to matrix elasticity 17 Thank You 18 Microscopic elasticity Random fibers Aligned fibers All boundaries fixed Two boundaries fixed • Elasticity experienced by the cells is dependent on the location of cell on the matrix direction applied boundary conditions 21 Cell-matrix interaction: location • Cell experiences substrate stiffness in of terms of work done for substrate deformation • This work done is also known as “self-energy of the cell” Random fibrous matrix a b c c α a b c b b a c b b a • Near the boundaries of the random fibrous matrix- anisotropic elasticity • For clamped-free-clamped-free boundary condition – whole matrix is anisotropic Anisotropic substrate Bischofs, I. B. et al, 2003, PNAS; Bischofs, I. B. et al, 2004, PRE Saez, A. et al., 2007, PNAS. Isotropic substrate 22 Effect of fiber alignment Aligned fibers α • Fiber alignment leads to anisotropic elasticity of fibrous matrix Experiments Random fibers Saha, S. et al., 2012, Langmuir Teh, T.K.H. et al., 2012, Tissue Engg. Part A Aligned fibers Effect of boundary conditions Free edge Fixed edge • Self energy of a cell is- • high near a fixed edge of random fibrous matrix • low near a free edge of random fibrous matrix Near free edge Near fixed edge • Boundary conditions of fibrous matrix can influence the cell behavior Grinnell, F., 2000, Trends in Cell Biol. Summary 1. Model • Fiber bending is not negligible for cell-matrix interaction • Fiber bending demonstrates strain stiffening and strain softening in fiber elongation and compression, respectively • Fiber fusion leads to stiffer matrix response 2. Cell-matrix interaction • Matrix stiffness experienced by the cell is dependent on the cell location, orientation, and matrix boundary conditions • Cellular forces cause fiber remodeling in the fibrous matrix • Fiber alignment leads to anisotropic mechanical properties of the matrix 3. Cell-cell interaction • Fibers align in the region between two cells • Cell-cell interaction depends on the cell orientations and the separation between them 25 Model parameters • Fiber diameter (a) • All fibers are not of same diameter • But the diameter of a fiber does not change with its length • aeffective ~ 1μm • Constitutive relation for fiber material (τ(γf )) • During mechanical testing large strains are applied • Large strains lead to stretching of fibers • Bending/Stretching ~ a2 ~ 10 -12 • Therefore, fiber bending can be ignored 0 Curved fiber τ • linear viscoelastic for dynamic loading τfr • Fiber breaks when stress in the fiber exceeds a threshold value Straight load • Before breaking, fiber response is bearing fiber • linear elastic for quasi-static loading Fiber breakage ε0 εfr Strain of the fibrous matrix Cell-matrix interactions • Cells apply localized forces to the substrate via focal adhesions. Focal adhesion Stress fiber Substrate • The modeling framework presented till now is not applicable • The understanding of behavior of the fibrous matrices against localized forces is needed Burridge, K. et al., 2013, J. Cell. Biol. Balaban, N. Q. et al., 2001, Nature Cell Biology Gjorevski, N. et al., 2012, Biophys. J. 27
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