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An interrelation between creep and relaxation is therefore developed for ligament viscoelasticity based on a single-integral nonlinear superposition model. This interrelation differs from the convolution relation obtained by Laplace transforms for linear materials. We demonstrate via continuum concepts of nonlinear viscoelasticity that such a difference in rate between creep and relaxation phenomenologically occurs when the nonlinearity is of a strain-stiffening type, i.e. the stress-strain curve is concave up as observed in ligament. We also show that it is inconsistent to assume a Fung-type constitutive law (Fung, 1972) for both creep and relaxation in ligament viscoelasticity. Using published data of Thornton, et al., the nonlinear interrelation developed herein predicts creep behavior from relaxation data well (R greater than 0.998). Although data are limited and the causal mechanisms associated with viscoelastic tissue behavior are complex, continuum concepts demonstrated here appear capable of interrelating creep and relaxation with fidelity. The image shows ligament structure, after Vanderby.
The research is primarily directed toward study of nonlinearly viscoelastic behavior of soft connective tissues, particularly the constitutive behavior representing ligament viscoelasticity. Because of their simplicity, ligaments are chosen as an experimental model. The research is organized as follows. (i) An experimental study is in progress, that defines viscoelastic behavior throughout the range of reversible ligament deformations. This study uses creep and relaxation plus recovery protocols to allow discrimination among various nonlinearities. (ii) A robust viscoelastic constitutive model is developed from experimental data. This model appropriately accounts for nonlinearities and interrelates creep and relaxation. (iii) The reversible deformation limits for levels of applied stress and strain (as a function of load-time) is experimentally identified from the data in (i), thus defining the onset of sub-failure tissue damage for a single overload. A sub-failure criterion for the onset of damage is then formulated. (iv) Creep and relaxation testing are performed on additional specimens to quantify the compromise in mechanical behavior after higher loadings and deformations produce greater levels of tissue damage (from a single overload). (v) The microtrauma and damage associated with irreversible deformations is morphologically characterized using scanning electron microscopy.|
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