High-order X-FEM for the simulation of sound absorbing poro-elastic materials with coupling interfaces

Abstract In this paper, the acoustic field with the presence of poro-elastic materials is simulated by the eXtended Finite Element Method (X-FEM). Problems involving interfaces between different media are our main focus. The proposed method allows interfaces to be embedded in the finite elements, easing significantly the discretization, especially when the geometry of the interface is complex. The gradient discontinuity at the interface is handled through the ridge enrichment function. The strategies of spatial discretization for two different types of coupling interface are provided. A high-order approximation is used to improve the rate of convergence for the Biot mixed formulation ( u s , p ) and to eliminate the pollution effect at high frequencies. The verification of the method is performed with two benchmarks. Convergences of the solutions exhibit the capability and the accuracy of the present method under different conditions: coupling types, geometric complexity and a wide range of frequency. The applicability and advantage of the method in practical situations are demonstrated by a car cavity problem where part of the geometry is modified without re-meshing. This paper demonstrates that high-order X-FEM is an efficient computational approach for analysing sound-absorbing poro-elastic materials involving complex geometries.

[1]  Ted Belytschko,et al.  Structured extended finite element methods for solids defined by implicit surfaces , 2002 .

[2]  W. Wall,et al.  An eXtended Finite Element Method/Lagrange multiplier based approach for fluid-structure interaction , 2008 .

[3]  O. Cessenat,et al.  Application of an Ultra Weak Variational Formulation of Elliptic PDEs to the Two-Dimensional Helmholtz Problem , 1998 .

[4]  T. Belytschko,et al.  MODELING HOLES AND INCLUSIONS BY LEVEL SETS IN THE EXTENDED FINITE-ELEMENT METHOD , 2001 .

[5]  Olivier Dazel,et al.  A discontinuous Galerkin method with plane waves for sound‐absorbing materials , 2015 .

[6]  Benoit Nennig,et al.  The Partition of Unity Finite Element Method for the simulation of waves in air and poroelastic media. , 2014, The Journal of the Acoustical Society of America.

[7]  Ivo Babuška,et al.  The generalized finite element method for Helmholtz equation: Theory, computation, and open problems , 2006 .

[8]  Owe Axelsson,et al.  Superlinear convergence using block preconditioners for the real system formulation of complex Helmholtz equations , 2018, J. Comput. Appl. Math..

[9]  J. Allard Propagation of Sound in Porous Media: Modelling Sound Absorbing Materials , 1994 .

[10]  Nils-Erik Hörlin,et al.  A 3-D HIERARCHICAL FE FORMULATION OF BIOT'S EQUATIONS FOR ELASTO-ACOUSTIC MODELLING OF POROUS MEDIA , 2001 .

[11]  I. Babuska,et al.  The partition of unity finite element method: Basic theory and applications , 1996 .

[12]  Grégory Legrain,et al.  High order X-FEM and levelsets for complex microstructures: Uncoupling geometry and approximation , 2012 .

[13]  Joel Koplik,et al.  Theory of dynamic permeability and tortuosity in fluid-saturated porous media , 1987, Journal of Fluid Mechanics.

[14]  D. Arnold An Interior Penalty Finite Element Method with Discontinuous Elements , 1982 .

[15]  I. Babuska,et al.  Dispersion and pollution of the FEM solution for the Helmholtz equation in one, two and three dimensions , 1999 .

[16]  Ted Belytschko,et al.  A finite element method for crack growth without remeshing , 1999 .

[17]  Wim Desmet,et al.  A Wave Based Method for the efficient solution of the 2D poroelastic Biot equations , 2012 .

[18]  Raymond Panneton,et al.  A mixed displacement-pressure formulation for poroelastic materials , 1998 .

[19]  Olivier Dazel,et al.  An alternative Biot's displacement formulation for porous materials. , 2007, The Journal of the Acoustical Society of America.

[20]  Benoit Nennig,et al.  The method of fundamental solutions for acoustic wave scattering by a single and a periodic array of poroelastic scatterers , 2011 .

[21]  Peter Göransson,et al.  A normal modes technique to reduce the order of poroelastic models: application to 2D and coupled 3D models , 2013 .

[22]  Jean-François Remacle,et al.  A computational approach to handle complex microstructure geometries , 2003 .

[23]  Nils-Erik Hörlin,et al.  3D hierarchical hp-FEM applied to elasto-acoustic modelling of layered porous media , 2005 .

[24]  Peter Hansbo,et al.  Nitsche's method for coupling non-matching meshes in fluid-structure vibration problems , 2003 .

[25]  Werley G. Facco,et al.  Handling material discontinuities in a nonconforming generalized finite element method to solve wave propagation problems , 2012 .

[26]  Yvan Champoux,et al.  Dynamic tortuosity and bulk modulus in air‐saturated porous media , 1991 .

[27]  Antoine Legay,et al.  The extended finite element method combined with a modal synthesis approach for vibro‐acoustic problems , 2015 .

[28]  Hadrien Bériot,et al.  A comparison of high-order polynomial and wave-based methods for Helmholtz problems , 2016, J. Comput. Phys..

[29]  Noureddine Atalla,et al.  Convergence of poroelastic finite elements based on Biot displacement formulation , 2001 .

[30]  Grégory Legrain,et al.  A NURBS enhanced extended finite element approach for unfitted CAD analysis , 2013 .

[31]  M. Biot MECHANICS OF DEFORMATION AND ACOUSTIC PROPAGATION IN POROUS MEDIA , 1962 .

[32]  Nicolas Moës,et al.  Studied X-FEM enrichment to handle material interfaces with higher order finite element , 2010 .

[33]  M. Biot Theory of Propagation of Elastic Waves in a Fluid‐Saturated Porous Solid. I. Low‐Frequency Range , 1956 .

[34]  E. Perrey-Debain,et al.  Performances of the Partition of Unity Finite Element Method for the analysis of two-dimensional interior sound fields with absorbing materials , 2013 .