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    A Triphasic Theory for the Swelling and Deformation Behaviors of Articular Cartilage

    Source: Journal of Biomechanical Engineering:;1991:;volume( 113 ):;issue: 003::page 245
    Author:
    W. M. Lai
    ,
    J. S. Hou
    ,
    V. C. Mow
    DOI: 10.1115/1.2894880
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: Swelling of articular cartilage depends on its fixed charge density and distribution, the stiffness of its collagen-proteoglycan matrix, and the ion concentrations in the interstitium. A theory for a tertiary mixture has been developed, including the two fluid-solid phases (biphasic), and an ion phase, representing cation and anion of a single salt, to describe the deformation and stress fields for cartilage under chemical and/or mechanical loads. This triphasic theory combines the physico-chemical theory for ionic and polyionic (proteoglycan) solutions with the biphasic theory for cartilage. The present model assumes the fixed charge groups to remain unchanged, and that the counter-ions are the cations of a single salt of the bathing solution. The momentum equation for the neutral salt and for the intersitial water are expressed in terms of their chemical potentials whose gradients are the driving forces for their movements. These chemical potentials depend on fluid pressure p, salt concentration c, solid matrix dilatation e and fixed charge density cF . For a uni-uni valent salt such as NaCl, they are given by μi = μo i + (RT/Mi )ln[γ± 2 c (c + c F )] and μW = μo w + [p − RTφ(2c + cF ) + Bw e]/ρT w , where R, T, Mi , γ± , φ, ρT w and Bw are universal gas constant, absolute temperature, molecular weight, mean activity coefficient of salt, osmotic coefficient, true density of water, and a coupling material coefficient, respectively. For infinitesimal strains and material isotropy, the stress-strain relationship for the total mixture stress is σ = − pI − Tc I + λs (trE)I + 2μs E, where E is the strain tensor and (λs ,μs ) are the Lamé constants of the elastic solid matrix. The chemical-expansion stress (− Tc ) derives from the charge-to-charge repulsive forces within the solid matrix. This theory can be applied to both equilibrium and non-equilibrium problems. For equilibrium free swelling problems, the theory yields the well known Donnan equilibrium ion distribution and osmotic pressure equations, along with an analytical expression for the “pre-stress” in the solid matrix. For the confined-compression swelling problem, it predicts that the applied compressive stress is shared by three load support mechanisms: 1) the Donnan osmotic pressure; 2) the chemical-expansion stress; and 3) the solid matrix elastic stress. Numerical calculations have been made, based on a set of equilibrium free-swelling and confined-compression data, to assess the relative contribution of each mechanism to load support. Our results show that all three mechanisms are important in determining the overall compressive stiffness of cartilage.
    keyword(s): Deformation , Cartilage , Stress , Equilibrium (Physics) , Density , Mechanisms , Mixtures , Stiffness , Water , Force , Pressure , Chemical potential , Compression , Equations , Gradients , Isotropy , Compressive stress , Tensors , Stress-strain relations , Constants (Physics) , Momentum , Fluid pressure , Temperature , Ions , Fluids , Motion AND Molecular weight ,
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      A Triphasic Theory for the Swelling and Deformation Behaviors of Articular Cartilage

    URI
    http://yetl.yabesh.ir/yetl1/handle/yetl/108154
    Collections
    • Journal of Biomechanical Engineering

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    contributor authorW. M. Lai
    contributor authorJ. S. Hou
    contributor authorV. C. Mow
    date accessioned2017-05-08T23:34:51Z
    date available2017-05-08T23:34:51Z
    date copyrightAugust, 1991
    date issued1991
    identifier issn0148-0731
    identifier otherJBENDY-25873#245_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/108154
    description abstractSwelling of articular cartilage depends on its fixed charge density and distribution, the stiffness of its collagen-proteoglycan matrix, and the ion concentrations in the interstitium. A theory for a tertiary mixture has been developed, including the two fluid-solid phases (biphasic), and an ion phase, representing cation and anion of a single salt, to describe the deformation and stress fields for cartilage under chemical and/or mechanical loads. This triphasic theory combines the physico-chemical theory for ionic and polyionic (proteoglycan) solutions with the biphasic theory for cartilage. The present model assumes the fixed charge groups to remain unchanged, and that the counter-ions are the cations of a single salt of the bathing solution. The momentum equation for the neutral salt and for the intersitial water are expressed in terms of their chemical potentials whose gradients are the driving forces for their movements. These chemical potentials depend on fluid pressure p, salt concentration c, solid matrix dilatation e and fixed charge density cF . For a uni-uni valent salt such as NaCl, they are given by μi = μo i + (RT/Mi )ln[γ± 2 c (c + c F )] and μW = μo w + [p − RTφ(2c + cF ) + Bw e]/ρT w , where R, T, Mi , γ± , φ, ρT w and Bw are universal gas constant, absolute temperature, molecular weight, mean activity coefficient of salt, osmotic coefficient, true density of water, and a coupling material coefficient, respectively. For infinitesimal strains and material isotropy, the stress-strain relationship for the total mixture stress is σ = − pI − Tc I + λs (trE)I + 2μs E, where E is the strain tensor and (λs ,μs ) are the Lamé constants of the elastic solid matrix. The chemical-expansion stress (− Tc ) derives from the charge-to-charge repulsive forces within the solid matrix. This theory can be applied to both equilibrium and non-equilibrium problems. For equilibrium free swelling problems, the theory yields the well known Donnan equilibrium ion distribution and osmotic pressure equations, along with an analytical expression for the “pre-stress” in the solid matrix. For the confined-compression swelling problem, it predicts that the applied compressive stress is shared by three load support mechanisms: 1) the Donnan osmotic pressure; 2) the chemical-expansion stress; and 3) the solid matrix elastic stress. Numerical calculations have been made, based on a set of equilibrium free-swelling and confined-compression data, to assess the relative contribution of each mechanism to load support. Our results show that all three mechanisms are important in determining the overall compressive stiffness of cartilage.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleA Triphasic Theory for the Swelling and Deformation Behaviors of Articular Cartilage
    typeJournal Paper
    journal volume113
    journal issue3
    journal titleJournal of Biomechanical Engineering
    identifier doi10.1115/1.2894880
    journal fristpage245
    journal lastpage258
    identifier eissn1528-8951
    keywordsDeformation
    keywordsCartilage
    keywordsStress
    keywordsEquilibrium (Physics)
    keywordsDensity
    keywordsMechanisms
    keywordsMixtures
    keywordsStiffness
    keywordsWater
    keywordsForce
    keywordsPressure
    keywordsChemical potential
    keywordsCompression
    keywordsEquations
    keywordsGradients
    keywordsIsotropy
    keywordsCompressive stress
    keywordsTensors
    keywordsStress-strain relations
    keywordsConstants (Physics)
    keywordsMomentum
    keywordsFluid pressure
    keywordsTemperature
    keywordsIons
    keywordsFluids
    keywordsMotion AND Molecular weight
    treeJournal of Biomechanical Engineering:;1991:;volume( 113 ):;issue: 003
    contenttypeFulltext
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