Design of phononic band gaps in functionally graded piezocomposite materials by using topology optimization

One of the properties of composite materials is the possibility of having phononic band gaps, within which sound and vibrations at certain frequencies do not propagate. These materials are called Phononic Crystals (PCs). PCs with large band gaps are of great interest for many applications, such as transducers, elastic/ acoustic filters, noise control, and vibration shields. Most of previous works concentrates on PCs made of elastic isotropic materials; however, band gaps can be enlarged by using non-isotropic materials, such as piezoelectric materials. Since the main property of PCs is the presence of band gaps, one possible way to design structures which have a desired band gap is through Topology Optimization Method (TOM). TOM is a computational technique that determines the layout of a material such that a prescribed objective is maximized. Functionally Graded Materials (FGM) are composite materials whose properties vary gradually and continuously along a specific direction within the domain of the material. One of the advantages of applying the FGM concept to TOM is that it is not necessary a discrete 0-1 result, once the material gradation is part of the solution. Therefore, the interpretation step becomes easier and the dispersion diagram obtained from the optimization is not significantly modified. In this work, the main objective is to optimize the position and width of piezocomposite materials band gaps. Finite element analysis is implemented with Bloch-Floquet theory to solve the dynamic behavior of two-dimensional functionally graded unit cells. The results demonstrate that phononic band gaps can be designed by using this methodology.

[1]  K. Svanberg The method of moving asymptotes—a new method for structural optimization , 1987 .

[2]  K. Matsui,et al.  Continuous approximation of material distribution for topology optimization , 2004 .

[3]  Gregory M. Hulbert,et al.  Multiobjective evolutionary optimization of periodic layered materials for desired wave dispersion characteristics , 2006 .

[4]  Glaucio H. Paulino,et al.  Optimal design of periodic functionally graded composites with prescribed properties , 2009 .

[5]  N. Kikuchi,et al.  Design of piezocomposite materials and piezoelectric transducers using topology optimization— Part III , 1999 .

[6]  Ole Sigmund,et al.  Topology optimization: a tool for the tailoring of structures and materials , 2000, Philosophical Transactions of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences.

[7]  Sylvia R. Almeida,et al.  A simple and effective inverse projection scheme for void distribution control in topology optimization , 2009 .

[8]  James K. Guest,et al.  Achieving minimum length scale in topology optimization using nodal design variables and projection functions , 2004 .

[9]  Ole Sigmund,et al.  Systematic design of phononic band–gap materials and structures by topology optimization , 2003, Philosophical Transactions of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences.

[10]  Lien-Wen Chen,et al.  Elastic wave band gaps of one-dimensional phononic crystals with functionally graded materials , 2009 .

[11]  Z. Hou,et al.  Phononic crystals containing piezoelectric material , 2004 .

[12]  K. Kishimoto,et al.  Dispersion relations for SH-wave propagation in periodic piezoelectric composite layered structures , 2004 .

[13]  Glaucio H. Paulino,et al.  Topology optimization design of functionally graded bimorph-type piezoelectric actuators , 2007 .

[14]  Yukihiro Tanaka,et al.  Band structure of acoustic waves in phononic lattices: Two-dimensional composites with large acoustic mismatch , 2000 .