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A constitutive model for fibrous tissues considering collagen fiber crimp

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It is shown that the fiber crimp model can reproduce several of the expected characteristics of fibrous tissues and quantify the effect of parameter changes on the mechanical response.
Abstract
A micromechanically based constitutive model for fibrous tissues is presented. The model considers the randomly crimped morphology of individual collagen fibers, a morphology typically seen in photomicrographs of tissue samples. It describes the relationship between the fiber endpoints and its arc-length in terms of a measurable quantity, which can be estimated from image data. The collective mechanical behavior of collagen fibers is presented in terms of an explicit expression for the strain-energy function, where a fiber-specific random variable is approximated by a Beta distribution. The model-related stress and elasticity tensors are provided. Two representative numerical examples are analyzed with the aim of demonstrating the peculiar mechanism of the constitutive model and quantifying the effect of parameter changes on the mechanical response. In particular, a fibrous tissue, assumed to be (nearly) incompressible, is subject to a uniaxial extension along the fiber direction, and, separately, to pure shear. It is shown that the fiber crimp model can reproduce several of the expected characteristics of fibrous tissues.

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A constitutive model for brous tissues considering
collagen ber crimp
F. Cacho, P.J. Elbischger, J.F. Rodríguez, M. Doblaré, G.A. Holzapfel
To cite this version:
F. Cacho, P.J. Elbischger, J.F. Rodríguez, M. Doblaré, G.A. Holzapfel. A constitutive model for brous
tissues considering collagen ber crimp. International Journal of Non-Linear Mechanics, Elsevier, 2007,
42 (2), pp.391. �10.1016/j.ijnonlinmec.2007.02.002�. �hal-00501746�

www.elsevier.com/locate/nlm
Author’s Accepted Manuscript
A constitutive model for fibrous tissues considering
collagen fiber crimp
F. Cacho, P.J. Elbischger, J.F. Rodríguez, M. Doblaré,
G.A. Holzapfel
PII: S0020-7462(07)00055-8
DOI: doi:10.1016/j.ijnonlinmec.2007.02.002
Reference: NLM 1340
To appear in: International Journal of Non-
Linear Mechanics
Received date: 30 December 2006
Revised date: 6 February 2007
Accepted date: 6 February 2007
Cite this article as: F. Cacho, P.J. Elbischger, J.F. Rodríguez, M. Doblaré and G.A.
Holzapfel, A constitutive model for fibrous tissues considering collagen fiber crimp, Inter-
national Journal of Non-Linear Mechanics (2007), doi:10.1016/j.ijnonlinmec.2007.02.002
This is a PDF file of an unedited manuscript that has been accepted for publication. As
a service to our customers we are providing this early version of the manuscript. The
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Accepted manuscript
A constitutive model for fibrous tissues
considering collagen ber crimp
F. Cacho
a,b
, P.J. Elbischger
c
,J.F.Rodr´ıguez
b
M. Doblar´e
b
and G.A. Holzapfel
d,e
a
Institute for Structural Analysis, Computational Biomechanics
Graz University of Technology, Austria
b
Group of Structural Mechanics and Materials Modeling
Aragon Institute of Engineering Research (I3A), University of Zaragoza, Spain
c
Medical Information Technology, Carinthia Tech Institute
University of Applied Sciences, Klagenfurt, Austria
d
Department of Solid Mechanics, School of Engineering Sciences
Royal Institute of Technology (KTH), Stockholm, Sweden
e
Institute for Biomechanics, Graz University of Technology, Austria
Abstract
A micromechanically-based constitutive model for fibrous tissues is presented. The
model considers the randomly crimped morphology of individual collagen fibers, a
morphology typically seen in photomicrographs of tissue samples. It describes the
relationship between the ber endpoints and its arc-length in terms of a measur-
able quantity, which can be estimated from image data. The collective mechanical
behavior of collagen bers is presented in terms of an explicit expression for the
strain-energy function, where a fiber-specific random variable is approximated by a
Beta distribution. The model-related stress and elasticity tensors are provided. Two
representative numerical examples are analyzed with the aim of demonstrating the
peculiar mechanism of the constitutive model and quantifying the effect of param-
eter changes on the mechanical response. In particular, a brous tissue, assumed
to be (nearly) incompressible, is subject to a uniaxial extension along the ber di-
rection, and, separately, to pure shear. It is shown that the fiber crimp model can
reproduce several of the expected characteristics of fibrous tissues.
Key words: Collagen fiber, constitutive model, fiber crimp, micromechanics,
statistical distribution.
Corresponding author. Institute for Biomechanics, Center for Biomedical
Engineering, Graz University of Technology, Kronesgasse 5, 8010 Graz, Austria.
E-mail address: gh@biomech.tu-graz.ac.at (G.A. Holzapfel).
Preprint submitted to Elsevier Science 6 February 2007

Accepted manuscript
1 Introduction
The 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 mechan-
ical 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].
On the basis of the mechanical properties, a number of constitutive mod-
els have been developed in the past in attempts to describe the experimental
data. 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. The basic ideas of the theory are contained
in [12], with further developments on strongly anisotropic solids in [13], and
applications to model, e.g., arterial walls in [14,15]; see also the recent vol-
ume [16]. In such macroscopic models the collagen fibers are assumed to be
continuously arranged in the matrix material, as utilized in [17], and the char-
acteristic nonlinear stiffening is best represented by means of an exponential
function. Effective alternatives are based on limiting chain models, see, for
example, [18], and references therein.
The pioneering work by Lanir [19,20] on the mechanics of fibrous (connec-
tive) tissues as a consequence of its microstructure has influenced much of the
works on microstructural constitutive models. Essentially, the works [19,20]
postulate that the fibers are crimped and that they have different lengths so
that for a given macroscopic deformation in the material each individual fiber
is stretched differently. There is, thus, a distribution in either the stretch of
the fibers or their lengths. This idea has also been adopted subsequently by
means of constitutive models to describe the mechanical response of, e.g., ar-
terial walls ([21] with ideas from [22,14]) or tendons and ligaments [23], just
to name a few. All these constitutive models, however, assume unbounded
statistical distributions for the fiber length (or stretch), which is a bounded
quantity. In addition, in these models no attempt has been made to correlate
the fiber morphology (crimp) with the associated mechanical response in the
form of stress-stretch relationships. It was Lanir who considered the possibility
that the stretch could be nonuniform due to crimping, with a generic distri-
bution along the fiber axis, which he assumed to be Gaussian. Recently, Freed
and Doehring [24] have proposed a model where crimped fibrils in a fascicle
are approximated as a helical spring. Thereby, the collagen fiber waveforms
have a pre-defined arrangement; no statistical distribution is used. In differ-
ent works, such as [25–27], the distribution of the fiber orientations has been
addressed; however, therein, the mechanical properties of the collagen fibers
2

Accepted manuscript
within the tissue were considered to be independent of the degree of crimping.
In this paper a new constitutive model for the macroscopic behavior of fi-
brous tissues is presented. It takes the randomly crimped morphology of the
individual collagen fibers into account. In Section 2 a statistical description
of the fiber crimp is developed, which is used in Section 3 to model the col-
lective behavior of fibers. In Section 4 the mechanical behavior of a fibrous
tissue, assumed to be (nearly) incompressible, is analyzed in detail. The tissue
is subject to a stretch-controlled uniaxial extension along the fiber direction,
and, separately, to pure shear. In particular, the effect of the different model
parameters on the mechanical response is studied. The final section contains a
brief discussion together with a description of some limitations of the proposed
constitutive model.
2 Statistical and constitutive description of a single collagen fiber
In unloaded tissue samples collagen fibers show a wavy structure. In this
section we develop amodelthatincorporates the random crimp of collagen
fibers to be characterized.
2.1 Random crimp of a single fiber
We start by considering a set of randomly generated data in an interval of
length L
0
+ w on the X-axis such that at any point x within that interval
the associated coordinates y and z are independent and normally distributed
random variables with zero mean. Under this condition the data generated
can be regarded as white Gaussian noise, and characterized by the variance
σ
2
. In the following it is assumed that the variances in the Y and Z-directions
are equal, in other words the fiber undulates with equal characteristics in all
directions orthogonal to the X-axis.
The randomness of the data generated may be larger than that of an actual
fiber. By applying a smoothing function or filter h, which averages the coordi-
nates of the points in a neighborhood [w/2,w/2] of each point, a derived set
of data in the interval [0,L
0
] is obtained. It is implicitly assumed that h and
its first derivative has compact support in [w/2,w/2]. The resulting data
are also random and normally distributed with zero mean since the filtering
operation does not affect the Gaussian nature of the distribution. As a con-
sequence, the variance of the new random variable is unequivocally related to
that of the white Gaussian noise through the filter.
3

Citations
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Experimental investigation of collagen waviness and orientation in the arterial adventitia using confocal laser scanning microscopy.

TL;DR: Information on collagen fiber waviness and orientation could be used to develop structural models of the adventitia, providing better means for analyzing and understanding the mechanical properties of vascular wall.
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Hyperelastic Energy Densities for Soft Biological Tissues: A Review

TL;DR: A review of these constitutive equations can be found in this article, where the authors propose a review of the literature on constitutive models for soft tissues. But they do not consider the model that describes the behavior of the material.
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An anisotropic, hyperelastic model for skin: experimental measurements, finite element modelling and identification of parameters for human and murine skin.

TL;DR: A finite element model was developed using the transversely isotropic, hyperelastic constitutive model of Weiss et al. (1996) and was able to represent the nonlinear, anisotropic behaviour of the skin well and permitted quantification of the mechanical differences between human and murine skin.
Journal ArticleDOI

Mechanics of biological networks: From the cell cytoskeleton to connective tissue

TL;DR: This review focuses on the current progress in the field, with a primer into the basic physics of individual filaments and the networks they form, and a discussion of biological networks in the context of a broad spread of recent in vitro and in vivo experiments.
Journal ArticleDOI

Constitutive modeling of crimped collagen fibrils in soft tissues.

TL;DR: The proposed model is derived from the nonlinear axial force-stretch relationship of an extensible helical spring, including the full extension of the spring as a limit case, and only requires one material parameter and two geometrical parameters to be determined from experiments.
References
More filters
Journal ArticleDOI

Handbook of Mathematical Functions with Formulas

D. B. Owen
- 01 Feb 1965 - 
TL;DR: The Handbook of Mathematical Functions with Formulas (HOFF-formulas) as mentioned in this paper is the most widely used handbook for mathematical functions with formulas, which includes the following:
Journal ArticleDOI

A new constitutive framework for arterial wall mechanics and a comparative study of material models

TL;DR: In this paper, the authors developed a constitutive law for the description of the (passive) mechanical response of arterial tissue, where the artery is modeled as a thick-walled nonlinearly elastic circular cylindrical tube consisting of two layers corresponding to the media and adventitia.
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Nonlinear Solid Mechanics: A Continuum Approach for Engineering

TL;DR: In this paper, the authors introduce the concept of stress and balance principles for tensors and invariance of tensors in the context of Vectors and Tensors, and present a survey of the main aspects of objectivity.
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Frequently Asked Questions (13)
Q1. What are the contributions in "A constitutive model for fibrous tissues considering collagen fiber crimp" ?

A micromechanically-based constitutive model for fibrous tissues is presented. The collective mechanical behavior of collagen fibers is presented in terms of an explicit expression for the strain-energy function, where a fiber-specific random variable is approximated by a Beta distribution. The model-related stress and elasticity tensors are provided. Two representative numerical examples are analyzed with the aim of demonstrating the peculiar mechanism of the constitutive model and quantifying the effect of parameter changes on the mechanical response. 

In addition, the proposed model enables the derivation of analytical expressions while capturing the complexity of the tissue behavior. 

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]. 

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. 

the corresponding component of the structure tensor is zero and the stress contribution of the fibers in the X-direction vanishes. 

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. 

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. 

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. 

In the proposed approach the fibers must only be long enough with respect to their (random) wavelengths, which is the case for fibrous tissues. 

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,∞). 

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]). 

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. 

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.