An extended biphasic model for charged hydrated tissues with application to the intervertebral disc

被引:94
作者
Ehlers, W. [1 ]
Karajan, N. [1 ]
Markert, B. [1 ]
机构
[1] Univ Stuttgart, Inst Appl Mech Civil Engn, D-70569 Stuttgart, Germany
关键词
Intervertebral disc (IVD); Theory of Porous Media (TPM); Mixed FEM; Coupled problems; Anisotropy; Inhomogeneity; Finite viscoelasticity; Swelling; LUMBAR ANULUS FIBROSUS; FINITE-ELEMENT MODEL; ARTICULAR-CARTILAGE; POROUS-MEDIA; MECHANICAL-BEHAVIOR; ANNULUS FIBROSUS; MOTION SEGMENT; TENSILE PROPERTIES; NUCLEUS PULPOSUS; SOFT-TISSUES;
D O I
10.1007/s10237-008-0129-y
中图分类号
Q6 [生物物理学];
学科分类号
071011 [生物物理学];
摘要
Finite element models for hydrated soft biological tissue are numerous but often exhibit certain essential deficiencies concerning the reproduction of relevant mechanical and electro-chemical responses. As a matter of fact, singlephasic models can never predict the interstitial fluid flow or related effects like osmosis. Quite a few models have more than one constituent, but are often restricted to the small-strain domain, are not capable of capturing the intrinsic viscoelasticity of the solid skeleton, or do not account for a collagen fibre reinforcement. It is the goal of this contribution to overcome these drawbacks and to present a thermodynamically consistent model, which is formulated in a very general way in order to reproduce the behaviour of almost any charged hydrated tissue. Herein, the Theory of Porous Media (TPM) is applied in combination with polyconvex Ogden-type material laws describing the anisotropic and intrinsically viscoelastic behaviour of the solid matrix on the basis of a generalised Maxwell model. Moreover, other features like the deformation-dependent permeability, the possibility to include inhomogeneities like varying fibre alignment and behaviour, or osmotic effects based on the simplifying assumption of Lanir are also included. Finally, the human intervertebral disc is chosen as a representative for complex soft biological tissue behaviour. In this regard, two numerical examples will be presented with focus on the viscoelastic and osmotic capacity of the model.
引用
收藏
页码:233 / 251
页数:19
相关论文
共 102 条
[1]
[Anonymous], 9921 U STUTTG I MECH
[2]
[Anonymous], 1984, CALCOLO, DOI 10.1007/bf02576171
[3]
[Anonymous], 2000, THEORY POROUS MEDIA, DOI DOI 10.1007/978-3-642-59637-7
[4]
[Anonymous], 1984, Continuum Theory of the Mechanics of Fibre Reinforced Composites, DOI [10.1007/978-3-7091-4336-0_1, DOI 10.1007/978-3-7091-4336-0_1, 10.1007/978-3-7091-4336-0_, 10.1007/978-3-7091-4336-0, DOI 10.1007/978-3-7091-4336-0]
[5]
Poroelastic creep response analysis of a lumbar motion segment in compression [J].
Argoubi, M ;
ShiraziAdl, A .
JOURNAL OF BIOMECHANICS, 1996, 29 (10) :1331-1339
[6]
Ayad S., 1987, The Lumbar Spine and Back Pain, V3rd, P100
[7]
Direction-dependent constriction flow in a poroelastic solid: The intervertebral disc valve [J].
Ayotte, DC ;
Ito, K ;
Perren, SM ;
Tepic, S .
JOURNAL OF BIOMECHANICAL ENGINEERING-TRANSACTIONS OF THE ASME, 2000, 122 (06) :587-593
[8]
Incompressibility of the solid matrix of articular cartilage under high hydrostatic pressures [J].
Bachrach, NM ;
Mow, VC ;
Guilak, F .
JOURNAL OF BIOMECHANICS, 1998, 31 (05) :445-451
[9]
General theory of three-dimensional consolidation [J].
Biot, MA .
JOURNAL OF APPLIED PHYSICS, 1941, 12 (02) :155-164
[10]
Bishop A.W., 1959, TEKNISK UKEBLAD, V106, P859