A constitutive model for fibrous tissues considering collagen fiber crimp
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Citations
Experimental investigation of collagen waviness and orientation in the arterial adventitia using confocal laser scanning microscopy.
Hyperelastic Energy Densities for Soft Biological Tissues: A Review
An anisotropic, hyperelastic model for skin: experimental measurements, finite element modelling and identification of parameters for human and murine skin.
Mechanics of biological networks: From the cell cytoskeleton to connective tissue
Constitutive modeling of crimped collagen fibrils in soft tissues.
References
Handbook of Mathematical Functions with Formulas
A new constitutive framework for arterial wall mechanics and a comparative study of material models
Entropic elasticity of lambda-phage DNA
Nonlinear Solid Mechanics: A Continuum Approach for Engineering
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A new constitutive framework for arterial wall mechanics and a comparative study of material models
Frequently Asked Questions (13)
Q2. What is the advantage of the proposed model?
In addition, the proposed model enables the derivation of analytical expressions while capturing the complexity of the tissue behavior.
Q3. What is the role of collagen in mammalian tissue?
tThe central role of collagen as the major structural protein of mammalian tissue, comprising approximately one-third of the total protein in mammalian organisms, has motivated a significant effort towards determining its mechanical properties at all levels, ranging from single monomers [1,2] and long-chain polymers [3,4] to a structural element within a (macroscopic) biological tissue [5–8].
Q4. What is the popular theory of the macroscopic level?
While at the microscopic level, chain models such as the (Kratky-Porod) worm-like model are popular [9–11], at the macroscopic level the continuum theory of finite elastic deformations of solids reinforced with fibers is frequently the constitutive theory of choice.
Q5. What is the corresponding component of the structure tensor?
the corresponding component of the structure tensor is zero and the stress contribution of the fibers in the X-direction vanishes.
Q6. What is the way to capture the softening of the fiber?
On the basis of continuum mechanics the (macroscopic) constitutive model is formulated in terms of a few parameters, and it can capture material softening due to fiber failure.
Q7. What is the way to represent the mechanical properties of collagen fibers?
In such macroscopic models the collagen fibers are assumed to be continuously arranged in the matrix material, as utilized in [17], and the characteristic nonlinear stiffening is best represented by means of an exponential function.
Q8. What is the strain energy required to stretch the tissue?
If λ̄ increases beyond max(m, max) (beyond either full recruitment or mixed recruitment/failure) the strain energy required to stretch the tissue until complete failure (i.e. at λ̄ = m+ max) isψ= k2[ λ̄2−2mγλ̄η+γ +γ(γ+1)m2(η+γ)(η+γ+1)] +ψ̂, max(m, max)<λ̄≤m+ max.
Q9. What is the approach for a fibrous tissue?
In the proposed approach the fibers must only be long enough with respect to their (random) wavelengths, which is the case for fibrous tissues.
Q10. What is the probability density function of r?
A.1 Probability density function P ofFrom eq. (2) the authors know that = √ 2d2 + 1. Define now r = 2d2, which is a random variable whose distribution is χ2 with σd, and thusP(r) = 1 2σ2d exp ( − r 2σ2d ) , r ∈ [0,∞).
Q11. Why is the neo-Hookean model suitable for matr?
Although several models capable of describing large deformations are suitable for ψmatrix [33], it is common to apply the neo-Hookean model because of its simplicity (see, e.g., [17, Chapter 6]).
Q12. What is the axis of the fibers?
6. The fiber families are located in the X-Y plane, and are symmetrically disposed with respect to the X axis and described in terms of the angle θ.
Q13. What is the tensor for the neo-Hookean model?
The tensor Cvol in (31) is given in [17], p. 254, and Cmatrix reduces to the (fourth-order) zero tensor for the neo-Hookean model.