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Mathematical modeling of anisotropic hyperelastic cylindrical thick shells by incorporating thickness deformation and compressibility with application to arterial walls. (English) Zbl 1537.74260

Summary: This paper is devoted to mathematical modeling of anisotropic hyperelastic thick cylindrical shells like arteries by taking into account the volume compressibility and through-the-thickness deformation. To describe the hyperelastic behavior of this kind of shells and extract their constitutive relations, the modified anisotropic (MA) model is employed, which is able to characterize compressible behavior of hyperelastic materials like soft tissues. By considering the arterial segment as a thick cylindrical shell, the higher order thickness deformation shell theory together with nonlinear Green’s strains are exploited to express its deformations and capture the thickness stretching effect. The shell is then discretized via Lagrange equations of motion to achieve the responses of the arterial wall. Numerical results are given in two sections. First, the presented formulation is validated by conducting a comparative study on a single-layer compressible pressurized shell. Close agreement between the outcomes of the developed model with those provided by finite element (FE) simulation signifies the necessity of incorporating thickness deformation in the higher order shell theory. In the next step, by considering the artery as a two-layer cylindrical shell comprising the media (the middle layer of the artery) and the adventitia (the outer layer), mechanical responses of an arterial wall subjected to an internal pressure are appraised through a number of parametric studies.

MSC:

74K25 Shells
74S05 Finite element methods applied to problems in solid mechanics

Software:

MUL2
Full Text: DOI

References:

[1] Mooney, M., A theory of large elastic deformation, J. Appl. Phys.11(9) (1940) 582-592. · JFM 66.1021.04
[2] Blatz, P. J. and Ko, W. L., Application of finite elastic theory to the deformation of rubbery materials, Trans. Soc. Rheol.6(1) (1962) 223-252.
[3] Ogden, R. W., Large deformation isotropic elasticity-on the correlation of theory and experiment for incompressible rubberlike solids, Proc. R. Soc. Lond. A Math. Phys. Sci.326(1567) (1972) 565-584. · Zbl 0257.73034
[4] Yeoh, O. H., Some forms of the strain energy function for rubber, Rubber Chem. Technol.66(5) (1993) 754-771.
[5] Gent, A. N., A new constitutive relation for rubber, Rubber Chem. Technol.69(1) (1996) 59-61.
[6] Kim, H. G., A comparative study of hyperelastic and hypoelastic material models with constant elastic moduli for large deformation problems, Acta Mech.227(5) (2016) 1351-1362. · Zbl 1341.74151
[7] Chen, W., Wang, L. and Dai, H., Nonlinear free vibration of hyperelastic beams based on neo-Hookean model, Int. J. Struct. Stab. Dyn.20(1) (2020) 2050015. · Zbl 1535.74185
[8] Zhao, Z., Zhang, W., Zhang, H. and Yuan, X., Some interesting nonlinear dynamic behaviors of hyperelastic spherical membranes subjected to dynamic loads, Acta Mech.230(8) (2019) 3003-3018. · Zbl 1428.74131
[9] Xu, J., Yuan, X., Zhang, H., Zheng, F. and Chen, L., Nonlinear vibrations of thermo-hyperelastic moderately thick cylindrical shells with 2: 1 internal resonance, Int. J. Struct. Stab. Dyn.20(5) (2020) 2050067. · Zbl 1535.74322
[10] He, L., Lou, J., Dong, Y., Kitipornchai, S. and Yang, J., Variational modeling of plane-strain hyperelastic thin beams with thickness-stretching effect, Acta Mech.229(12) (2018) 4845-4861. · Zbl 1430.74022
[11] Zhang, J., Xu, J., Yuan, X., Zhang, W. and Niu, D., Strongly nonlinear vibrations of a hyperelastic thin-walled cylindrical shell based on the modified Lindstedt-Poincaré method, Int. J. Struct. Stab. Dyn.19(12) (2019) 1950160.
[12] Bacciocchi, M. and Tarantino, A. M., Bending of hyperelastic beams made of transversely isotropic material in finite elasticity, Appl. Math. Model.100 (2021) 55-76. · Zbl 1481.74072
[13] Tang, D., Lim, C. W., Hong, L., Jiang, J. and Lai, S. K., Dynamic response and stability analysis with Newton harmonic balance method for nonlinear oscillating dielectric elastomer balloons, Int. J. Struct. Stab. Dyn.18(12) (2018) 1850152. · Zbl 1535.74382
[14] Bacciocchi, M. and Tarantino, A. M., Finite bending of hyperelastic beams with transverse isotropy generated by longitudinal porosity, Eur. J. Mech. A Solids85 (2021) 104131. · Zbl 1476.74086
[15] Shojaeifard, M., Sheikhi, S., Baniassadi, M. and Baghani, M., On finite bending of visco-hyperelastic materials: A novel analytical solution and FEM, Acta Mech.231(8) (2020) 3435-3450. · Zbl 1440.74071
[16] Gou, K. and Muddamallappa, M. S., An analytic study on nonlinear radius change for hyperelastic tubular organs under volume expansion, Acta Mech.231 (2020) 1-15. · Zbl 1440.74225
[17] Chaimoon, K. and Chindaprasirt, P., An anisotropic hyperelastic model with an application to soft tissues, Eur. J. Mech. A Solids78 (2019) 103845. · Zbl 1473.74012
[18] Ahearne, M., Yang, Y., Then, K. Y. and Liu, K. K., An indentation technique to characterize the mechanical and viscoelastic properties of human and porcine corneas, Ann. Biomed. Eng.35(9) (2007) 1608-1616.
[19] Pandolfi, A. and Holzapfel, G. A., Three-dimensional modeling and computational analysis of the human cornea considering distributed collagen fibril orientations, J. Biomech. Eng.130(6) (2008).
[20] Asher, R., Gefen, A., Moisseiev, E. and Varssano, D., An analytical approach to corneal mechanics for determining practical, clinically-meaningful patient-specific tissue mechanical properties in the rehabilitation of vision, Ann. Biomed. Eng.43(2) (2015) 274-286.
[21] Cheng, X. and Pinsky, P. M., A numerical model for metabolism, metabolite transport and edema in the human cornea, Comput. Methods Appl. Mech. Eng.314 (2017) 323-344. · Zbl 1439.74195
[22] Zhu, Z., Jiang, C. and Jiang, H., A visco-hyperelastic model of brain tissue incorporating both tension/compression asymmetry and volume compressibility, Acta Mech.230(6) (2019). · Zbl 1428.74158
[23] Comellas, E., Budday, S., Pelteret, J. P., Holzapfel, G. A. and Steinmann, P., Modeling the porous and viscous responses of human brain tissue behavior, Comput. Methods Appl. Mech. Eng.369 (2020) 113128. · Zbl 1506.74204
[24] Amabili, M., Breslavsky, I. D. and Reddy, J. N., Nonlinear higher-order shell theory for incompressible biological hyperelastic materials, Comput. Methods Appl. Mech. Eng.346 (2019) 841-861. · Zbl 1440.74063
[25] Soltani, H., Payette, G. S. and Reddy, J. N., Vibration of elastic beams in the presence of an inviscid fluid medium, Int. J. Struct. Stab. Dyn.14(6) (2014) 1450022. · Zbl 1359.74239
[26] Fok, P. W. and Gou, K., Finite element simulation of intimal thickening in 2D multi-layered arterial cross sections by morphoelasticity, Comput. Methods Appl. Mech. Eng.363 (2020) 112860. · Zbl 1436.74042
[27] Xie, J., Zhou, J. and Fung, Y. C., Bending of blood vessel wall: stress-strain laws of the intima-media and adventitial layers, J. Biomech. Eng.117(1) (1995) 136-145.
[28] Librescu, L., Refined geometrically nonlinear theories of anisotropic laminated shells, Quart. Appl. Math.45(1) (1987) 1-22. · Zbl 0632.73048
[29] Reddy, J. N., Exact solutions of moderately thick laminated shells, J. Eng. Mech.110(5) (1984) 794-809.
[30] Reddy, J. N. and Liu, C., A higher-order shear deformation theory of laminated elastic shells, Int. J. Eng. Sci.23(3) (1985) 319-330. · Zbl 0559.73072
[31] Dennis, S. T. and Palazotto, A. N., Large displacement and rotational formulation for laminated shells including parabolic transverse shear, Int. J. Non Linear Mech.25(1) (1990) 67-85. · Zbl 0704.73042
[32] Arciniega, R. A. and Reddy, J. N., Consistent third-order shell theory with application to composite cylindrical cylinders, AIAA J.43(9) (2005) 2024-2038.
[33] Sansour, C., A theory and finite element formulation of shells at finite deformations involving thickness change: Circumventing the use of a rotation tensor, Arch. Appl. Mech.65(3) (1995) 194-216. · Zbl 0827.73044
[34] Carrera, E., Brischetto, S., Cinefra, M. and Soave, M., Effects of thickness stretching in functionally graded plates and shells, Compos. B: Eng.42(2) (2011) 123-133.
[35] Ferreira, A. J. M., Carrera, E., Cinefra, M. and Roque, C. M. C., Analysis of laminated doubly-curved shells by a layerwise theory and radial basis functions collocation, accounting for through-the-thickness deformations, Comput. Mech.48(1) (2011) 13-25. · Zbl 1328.74051
[36] Amabili, M., Non-linearities in rotation and thickness deformation in a new third-order thickness deformation theory for static and dynamic analysis of isotropic and laminated doubly curved shells, Int. J. Non Linear Mech.69 (2015) 109-128.
[37] Fung, Y. C., Fronek, K. and Patitucci, P., Pseudoelasticity of arteries and the choice of its mathematical expression, Am. J. Physiol. Heart Circ. Physiol.237(5) (1979) H620-H631.
[38] Breslavsky, I. D., Amabili, M. and Legrand, M., Static and dynamic behavior of circular cylindrical shell made of hyperelastic arterial material, J. Appl. Mech.83(5) (2016) 52-68.
[39] Chuong, C. J. and Fung, Y. C., Three-dimensional stress distribution in arteries, J. Biomech. Eng.105(3) (1983) 268-274.
[40] Humphrey, J. D., Mechanics of the arterial wall: review and directions, Crit. Rev. Biomed. Eng.23(1-2) (1995) 22-37.
[41] Holzapfel, G. A., Gasser, T. C. and Ogden, R. W., A new constitutive framework for arterial wall mechanics and a comparative study of material models, J. Elast. Phys. Sci. Solids61(1-3) (2000) 1-48. · Zbl 1023.74033
[42] Holzapfel, G. A., Gasser, T. C. and Stadler, M., A structural model for the viscoelastic behavior of arterial walls: Continuum formulation and finite element analysis. Eur. J. Mech. A Solids21(3) (2002) 441-463. · Zbl 1100.74597
[43] Holzapfel, G. A., Stadler, M., Schulze-Bauer, C. A., A layer-specific three-dimensional model for the simulation of balloon angioplasty using magnetic resonance imaging and mechanical testing, Ann. Biomed. Eng.30(6) (2002) 753-767.
[44] Masson, I., Boutouyrie, P., Laurent, S., Humphrey, J. D. and Zidi, M., Characterization of arterial wall mechanical behavior and stresses from human clinical data, J. Biomech.41(12) (2008) 2618-2627.
[45] Stalhand, J., Determination of human arterial wall parameters from clinical data, Biomech. Model. Mechanobiol.8(2) (2009) 141-148.
[46] Tang, D.et al., 3D MRI-based anisotropic FSI models with cyclic bending for human coronary atherosclerotic plaque mechanical analysis, J. Biomech. Eng.131(6) (2009) 061010.
[47] Watton, P. N. and Hill, N. A., Evolving mechanical properties of a model of abdominal aortic aneurysm, Biomech. Model. Mech.8(1) (2009) 25-42.
[48] Kamenskiy, A.et al., Constitutive description of human femoropopliteal artery aging, Biomech. Model. Mechanobiol.16(2) (2017) 681-692.
[49] Gasser, T. C. and Holzapfel, G. A., A rate-independent elastoplastic constitutive model for biological fiber-reinforced composites at finite strains: Continuum basis, algorithmic formulation and finite element implementation, Comput. Mech.29(4-5) (2002) 340-360. · Zbl 1146.74342
[50] Gasser, T. C., Schulze-Bauer, C. A. and Holzapfel, G. A., A three-dimensional finite element model for arterial clamping, J. Biomech. Eng.124(4) (2002) 355-363.
[51] Hariton, I., Debotton, G., Gasser, T. C. and Holzapfel, G. A., Stress-driven collagen fiber remodeling in arterial walls, Biomech.Model. Mechanobiol.6(3) (2007) 163-175. · Zbl 1451.92047
[52] Rodriguez, J. F., Alastrue, V. and Doblare, M., Finite element implementation of a stochastic three dimensional finite-strain damage model for fibrous soft tissue, Comput. Methods Appl. Mech. Eng.197(9-12) (2008) 946-958. · Zbl 1169.74631
[53] Gasser, T. C., Ogden, R. W. and Holzapfel, G. A., Hyperelastic modelling of arterial layers with distributed collagen fibre orientations, J. R. Soc. Interface3(6) (2006) 15-35.
[54] Balzani, D., Brinkhues, S. and Holzapfel, G. A., Constitutive framework for the modeling of damage in collagenous soft tissues with application to arterial walls, Comput. Methods Appl. Mech. Eng.213 (2012) 139-151. · Zbl 1243.74119
[55] Pasta, S.et al., Constitutive modeling of ascending thoracic aortic aneurysms using microstructural parameters, Med. Eng. Phys.38(2) (2016) 121-130.
[56] Breslavsky, I. and Amabili, M., Nonlinear model of human descending thoracic aortic segments with residual stresses, Biomech. Model. Mechanobiol.17(6) (2018) 1839-1855.
[57] He, R., Zhao, L. G., Silberschmidt, V. V., Liu, Y. and Vogt, F., Finite element evaluation of artery damage in deployment of polymeric stent with pre-and post-dilation, Biomech. Model. Mechanobiol.19(1) (2020) 47-60.
[58] Nolan, D. R., Gower, A. L., Destrade, M., Ogden, R. W. and McGarry, J. P., A robust anisotropic hyperelastic formulation for the modelling of soft tissue, J. Mech. Behav. Biomed. Mater.39 (2014) 48-60.
[59] Amabili, M. and Reddy, J. N., A new non-linear higher-order shear deformation theory for large-amplitude vibrations of laminated doubly curved shells, Int. J. Non Linear Mech.45(4) (2010) 409-418.
[60] Amabili, M. and Breslavsky, I. D., Displacement dependent pressure load for finite deflection of doubly-curved thick shells and plates, Int. J. Non Linear Mech.77 (2015) 265-273.
[61] Nolan, D. R. and McGarry, J. P., On the compressibility of arterial tissue, Ann. Biomed. Eng.44(4) (2016) 993-1007.
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