TY - JOUR
T1 - An arbitrary Lagrangian-Eulerian method for simulating interfacial dynamics between a hydrogel and a fluid
AU - Li, Lei
AU - Zhang, Jiaqi
AU - Xu, Zelai
AU - Young, Y. N.
AU - Feng, James J.
AU - Yue, Pengtao
N1 - Funding Information:
J.Z. was partially supported by the National Science Foundation (Grants OAC-2015848 and EAR-1925575 ) and the Computational Infrastructure in Geodynamics initiative (through the National Science Foundation EAR-1550901 and the University of California – Davis). Y.-N.Y. acknowledges the financial support by the National Science Foundation (Grants DMS-1614863 and DMS-195160 ) and Flatiron Institute , part of Simons Foundation. J.J.F. acknowledges the financial support by the Natural Sciences and Engineering Research Council of Canada (Discovery Grant No. 2019-04162 ). P.Y. acknowledges the financial support by the National Science Foundation (Grant DMS-2012480 ). We thank Mattia Bacca for helpful discussions.
Funding Information:
J.Z. was partially supported by the National Science Foundation (Grants OAC-2015848 and EAR-1925575) and the Computational Infrastructure in Geodynamics initiative (through the National Science Foundation EAR-1550901 and the University of California ? Davis). Y.-N.Y. acknowledges the financial support by the National Science Foundation (Grants DMS-1614863 and DMS-195160) and Flatiron Institute, part of Simons Foundation. J.J.F. acknowledges the financial support by the Natural Sciences and Engineering Research Council of Canada (Discovery Grant No. 2019-04162). P.Y. acknowledges the financial support by the National Science Foundation (Grant DMS-2012480). We thank Mattia Bacca for helpful discussions.
Publisher Copyright:
© 2021 Elsevier Inc.
PY - 2022/2/15
Y1 - 2022/2/15
N2 - Hydrogels are crosslinked polymer networks swollen with an aqueous solvent, and play central roles in biomicrofluidic devices. In such applications, the gel is often in contact with a flowing fluid, thus setting up a fluid-hydrogel two-phase system. Using a recently proposed model (Young et al. [41] 2019), we treat the hydrogel as a poroelastic material consisting of a Saint Venant-Kirchhoff polymer network and a Newtonian viscous solvent, and develop a finite-element method for computing flows involving a fluid-hydrogel interface. The interface is tracked by using a fixed-mesh arbitrary Lagrangian-Eulerian method that maps the interface to a reference configuration. The interfacial deformation is coupled with the fluid and solid governing equations into a monolithic algorithm using the finite-element library deal.II. The code is validated against available analytical solutions in several non-trivial flow problems: one-dimensional compression of a gel layer by a uniform flow, two-layer shear flow, and the deformation of a Darcy gel particle in a planar extensional flow. In all cases, the numerical solutions are in excellent agreement with the analytical solutions. Numerical tests show second-order convergence with respect to mesh refinement, and first-order convergence with respect to time-step refinement.
AB - Hydrogels are crosslinked polymer networks swollen with an aqueous solvent, and play central roles in biomicrofluidic devices. In such applications, the gel is often in contact with a flowing fluid, thus setting up a fluid-hydrogel two-phase system. Using a recently proposed model (Young et al. [41] 2019), we treat the hydrogel as a poroelastic material consisting of a Saint Venant-Kirchhoff polymer network and a Newtonian viscous solvent, and develop a finite-element method for computing flows involving a fluid-hydrogel interface. The interface is tracked by using a fixed-mesh arbitrary Lagrangian-Eulerian method that maps the interface to a reference configuration. The interfacial deformation is coupled with the fluid and solid governing equations into a monolithic algorithm using the finite-element library deal.II. The code is validated against available analytical solutions in several non-trivial flow problems: one-dimensional compression of a gel layer by a uniform flow, two-layer shear flow, and the deformation of a Darcy gel particle in a planar extensional flow. In all cases, the numerical solutions are in excellent agreement with the analytical solutions. Numerical tests show second-order convergence with respect to mesh refinement, and first-order convergence with respect to time-step refinement.
KW - Fixed-mesh ALE method
KW - Fluid-structure interaction
KW - Hyperelasticity
KW - Permeability
KW - Poroelasticity model
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U2 - 10.1016/j.jcp.2021.110851
DO - 10.1016/j.jcp.2021.110851
M3 - Article
AN - SCOPUS:85119913125
SN - 0021-9991
VL - 451
JO - Journal of Computational Physics
JF - Journal of Computational Physics
M1 - 110851
ER -