2021
DOI: 10.1016/j.cma.2020.113494
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A thermodynamically consistent fractional visco-elasto-plastic model with memory-dependent damage for anomalous materials

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Cited by 32 publications
(23 citation statements)
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“…• Fractional calculus can be a interesting modeling alternative to describe the linear/nonlinear behavior of porcine UB especially within a material model selection framework, since fractional models potentially provide a reduced number of material parameters due to the presence of multiple power-laws in relaxation. Regarding potential future steps, investigating the possibility of plastic deformations under large strains by employing quasi-linear visco-plastic effects [61,62,63] and also failure mechanisms [7] would be interesting studies towards the life-cycle prediction of such anomalous bio-tissues. Finally the variation of tissue properties by anatomical location, orientation, and layers of the UB motivates further studies on distributed order models incorporating nonlinearities.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…• Fractional calculus can be a interesting modeling alternative to describe the linear/nonlinear behavior of porcine UB especially within a material model selection framework, since fractional models potentially provide a reduced number of material parameters due to the presence of multiple power-laws in relaxation. Regarding potential future steps, investigating the possibility of plastic deformations under large strains by employing quasi-linear visco-plastic effects [61,62,63] and also failure mechanisms [7] would be interesting studies towards the life-cycle prediction of such anomalous bio-tissues. Finally the variation of tissue properties by anatomical location, orientation, and layers of the UB motivates further studies on distributed order models incorporating nonlinearities.…”
Section: Discussionmentioning
confidence: 99%
“…The corresponding rheological symbol for the SB model represents a fractal-like arrangement of springs and dashpots [56,40], which we interpret as a compact, upscaled representation of a fractal-like microstructure. Regarding the thermodynamic admissibility of the SB element and more complex models (i.e., plasticity and damage) involving it, we refer the reader to Lion [36] for the SB model, and Suzuki et al [63]. The relaxation function G SB (t) [P a] for the SB model is given by the following single, inverse power-law form:…”
Section: First Stage: An Existence Study Of Fractional Linear Viscoel...mentioning
confidence: 99%
“…The corresponding rheological symbol for the SB model represents a fractal-like arrangement of springs and dashpots [7,56], which we interpret as a compact, upscaled representation of a fractal-like microstructure. Regarding the thermodynamic admissibility of the SB element and more complex models (i.e., plasticity and damage) involving it, we refer the reader to Lion [57] for the SB model, and Suzuki et al [58]. The relaxation function G SB (t) [Pa] for the SB model is given by the following single, inverse power-law form:…”
Section: First Stage: An Existence Study Of Fractional Linear Viscoel...mentioning
confidence: 99%
“…Regarding potential future steps, investigating the possibility of plastic deformations under large strains by employing quasi-linear visco-plastic effects [58,68,77] and also failure mechanisms [78] would be interesting studies towards the life-cycle prediction of such anomalous bio-tissues. Finally the variation of tissue properties by anatomical location, orientation, and layers of the UB motivates further studies on distributed order models incorporating nonlinearities.…”
mentioning
confidence: 99%
“…Here the fractional differential operator ∂ γ t := 0 I 1−γ t ∂ t for 0 ≤ γ < 1 with the fractional integral operator 0 I 1−γ t g := (t −γ /Γ(1 − γ)) * g and ∂ γ t := ∂ t u for γ = 1 [30]. Hence, the viscoelastic damping term −κ ∫ ∆Ω ∂ γ t udx accurately describes the behavior of viscoelastic damping, and includes the elastic resistance and viscoelastic damping as special cases [3,4,8,25,26,30,37,38], and has attracted growing research activities [9,11,13,17,18,21,24,28,31,32,41,42,44]. Consequently, the modeling equation becomes ∂ 2 t u(x, t) + κ∂ γ t u − K∇ 2 u(x, t) = f (x, t), (x, t) ∈ Ω × (0, T ], u(x, t) = 0, (x, t) ∈ ∂Ω × [0, T ]; u(x, 0) = u 0 (x), ∂ t u(x, 0) =ǔ 0 (x), x ∈ Ω,…”
Section: Introductionmentioning
confidence: 99%