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contributor authorD. D. Sun
contributor authorX. E. Guo
contributor authorM. Likhitpanichkul
contributor authorW. M. Lai
contributor authorV. C. Mow
date accessioned2017-05-09T00:12:21Z
date available2017-05-09T00:12:21Z
date copyrightFebruary, 2004
date issued2004
identifier issn0148-0731
identifier otherJBENDY-26353#6_1.pdf
identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/129643
description abstractUnconfined compression test has been frequently used to study the mechanical behaviors of articular cartilage, both theoretically and experimentally. It has also been used in explant and gel-cell-complex studies in tissue engineering. In biphasic and poroelastic theories, the effect of charges fixed on the proteoglycan macromolecules in articular cartilage is embodied in the apparent compressive Young’s modulus and the apparent Poisson’s ratio of the tissue, and the fluid pressure is considered to be the portion above the osmotic pressure. In order to understand how proteoglycan fixed charges might affect the mechanical behaviors of articular cartilage, and in order to predict the osmotic pressure and electric fields inside the tissue in this experimental configuration, it is necessary to use a model that explicitly takes into account the charged nature of the tissue and the flow of ions within its porous interstices. In this paper, we used a finite element model based on the triphasic theory to study how fixed charges in the porous-permeable soft tissue can modulate its mechanical and electrochemical responses under a step displacement in unconfined compression. The results from finite element calculations showed that: 1) A charged tissue always supports a larger load than an uncharged tissue of the same intrinsic elastic moduli. 2) The apparent Young’s modulus (the ratio of the equilibrium axial stress to the axial strain) is always greater than the intrinsic Young’s modulus of an uncharged tissue. 3) The apparent Poisson’s ratio (the negative ratio of the lateral strain to the axial strain) is always larger than the intrinsic Poisson’s ratio of an uncharged tissue. 4) Load support derives from three sources: intrinsic matrix stiffness, hydraulic pressure and osmotic pressure. Under the unconfined compression, the Donnan osmotic pressure can constitute between 13%–22% of the total load support at equilibrium. 5) During the stress-relaxation process following the initial instant of loading, the diffusion potential (due to the gradient of the fixed charge density and the associated gradient of ion concentrations) and the streaming potential (due to fluid convection) compete against each other. Within the physiological range of material parameters, the polarity of the electric potential depends on both the mechanical properties and the fixed charge density (FCD) of the tissue. For softer tissues, the diffusion effects dominate the electromechanical response, while for stiffer tissues, the streaming potential dominates this response. 6) Fixed charges do not affect the instantaneous strain field relative to the initial equilibrium state. However, there is a sudden increase in the fluid pressure above the initial equilibrium osmotic pressure. These new findings are relevant and necessary for the understanding of cartilage mechanics, cartilage biosynthesis, electromechanical signal transduction by chondrocytes, and tissue engineering.
publisherThe American Society of Mechanical Engineers (ASME)
titleThe Influence of the Fixed Negative Charges on Mechanical and Electrical Behaviors of Articular Cartilage Under Unconfined Compression
typeJournal Paper
journal volume126
journal issue1
journal titleJournal of Biomechanical Engineering
identifier doi10.1115/1.1644562
journal fristpage6
journal lastpage16
identifier eissn1528-8951
keywordsElasticity
keywordsElectric potential
keywordsBiological tissues
keywordsCompression
keywordsCartilage
keywordsPoisson ratio
keywordsPressure
keywordsStress
keywordsEquilibrium (Physics)
keywordsDisplacement
keywordsDensity
keywordsGradients
keywordsFinite element analysis AND Equations
treeJournal of Biomechanical Engineering:;2004:;volume( 126 ):;issue: 001
contenttypeFulltext


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