ebook img

Wave Propagation in Linear and Nonlinear Periodic Media: Analysis and Applications PDF

332 Pages·2012·6.167 MB·English
Save to my drive
Quick download
Download
Most books are stored in the elastic cloud where traffic is expensive. For this reason, we have a limit on daily download.

Preview Wave Propagation in Linear and Nonlinear Periodic Media: Analysis and Applications

CISM COURSES AND LECTURES Series Editors: The Rectors Friedrich Pfeiffer - Munich Franz G. Rammerstorfer - Wien Jean Salençon - Palaiseau The Secretary General (cid:2)(cid:3)(cid:4)(cid:5)(cid:6)(cid:7)(cid:4)(cid:8)(cid:9)(cid:10)(cid:11)(cid:6)(cid:4)(cid:3)(cid:12)(cid:3)(cid:4)(cid:9)(cid:13)(cid:9)(cid:14)(cid:7)(cid:8)(cid:15)(cid:7) Executive Editor (cid:14)(cid:7)(cid:16)(cid:17)(cid:16)(cid:9)(cid:10)(cid:3)(cid:4)(cid:7)(cid:18)(cid:5)(cid:19)(cid:9)(cid:13)(cid:9)(cid:20)(cid:8)(cid:19)(cid:5)(cid:3) The series presents lecture notes, monographs, edited works and (cid:21)(cid:4)(cid:16)(cid:11)(cid:3)(cid:3)(cid:8)(cid:19)(cid:5)(cid:22)(cid:23)(cid:9)(cid:19)(cid:5)(cid:9)(cid:24)(cid:6)(cid:3)(cid:9)(cid:18)(cid:3)(cid:17)(cid:8)(cid:9)(cid:16)(cid:25)(cid:9)(cid:26)(cid:3)(cid:11)(cid:6)(cid:7)(cid:5)(cid:19)(cid:11)(cid:23)(cid:27)(cid:9)(cid:28)(cid:5)(cid:22)(cid:19)(cid:5)(cid:3)(cid:3)(cid:4)(cid:19)(cid:5)(cid:22)(cid:27)(cid:9)(cid:29)(cid:16)(cid:30)(cid:21)(cid:15)(cid:24)(cid:3)(cid:4)(cid:9)(cid:10)(cid:11)(cid:19)(cid:3)(cid:5)(cid:11)(cid:3) and Applied Mathematics. (cid:14)(cid:15)(cid:4)(cid:21)(cid:16)(cid:23)(cid:3)(cid:9)(cid:16)(cid:25)(cid:9)(cid:24)(cid:6)(cid:3)(cid:9)(cid:23)(cid:3)(cid:4)(cid:19)(cid:3)(cid:23)(cid:9)(cid:19)(cid:23)(cid:9)(cid:24)(cid:16)(cid:9)(cid:30)(cid:7)(cid:31)(cid:3)(cid:9)(cid:31)(cid:5)(cid:16)!(cid:5)(cid:9)(cid:19)(cid:5)(cid:9)(cid:24)(cid:6)(cid:3)(cid:9)(cid:19)(cid:5)(cid:24)(cid:3)(cid:4)(cid:5)(cid:7)(cid:24)(cid:19)(cid:16)(cid:5)(cid:7)(cid:17)(cid:9)(cid:23)(cid:11)(cid:19)(cid:3)(cid:5)(cid:24)(cid:19)(cid:18)(cid:11) and technical community results obtained in some of the activities (cid:16)(cid:4)(cid:22)(cid:7)(cid:5)(cid:19)"(cid:3)(cid:8)(cid:9)#$(cid:9)(cid:29)%(cid:10)(cid:26)(cid:27)(cid:9)(cid:24)(cid:6)(cid:3)(cid:9)%(cid:5)(cid:24)(cid:3)(cid:4)(cid:5)(cid:7)(cid:24)(cid:19)(cid:16)(cid:5)(cid:7)(cid:17)(cid:9)(cid:29)(cid:3)(cid:5)(cid:24)(cid:4)(cid:3)(cid:9)(cid:25)(cid:16)(cid:4)(cid:9)(cid:26)(cid:3)(cid:11)(cid:6)(cid:7)(cid:5)(cid:19)(cid:11)(cid:7)(cid:17)(cid:9)(cid:10)(cid:11)(cid:19)(cid:3)(cid:5)(cid:11)(cid:3)(cid:23)& %’((cid:28))’*(%+’*/(cid:9)(cid:29)(cid:28)’()(cid:28)(cid:9)0+)(cid:9)(cid:26)(cid:28)(cid:29)1*’%(cid:29)*/(cid:9)(cid:10)(cid:29)%(cid:28)’(cid:29)(cid:28)(cid:10) (cid:29)+(cid:20))(cid:10)(cid:28)(cid:10)(cid:9)*’2(cid:9)/(cid:28)(cid:29)((cid:20))(cid:28)(cid:10)(cid:9)(cid:13)(cid:9)’(cid:16)&(cid:9)345 6*7(cid:28)(cid:9)(cid:14))+(cid:14)*8*(%+’(cid:9)%’(cid:9)/%’(cid:28)*)(cid:9)*’2(cid:9) ’+’/%’(cid:28)*)(cid:9)(cid:14)(cid:28))%+2%(cid:29)(cid:9)(cid:26)(cid:28)2%*(cid:9) *’*/9(cid:10)%(cid:10)(cid:9)*’2(cid:9)*(cid:14)(cid:14)/%(cid:29)*(%+’(cid:10) (cid:28)2%((cid:28)2(cid:9)(cid:2)9 0)*’(cid:29)(cid:28)(cid:10)(cid:29)+(cid:9))+(cid:26)(cid:28)+(cid:9) (cid:20)’%7(cid:28))(cid:10)%(9(cid:9);/*(cid:9)(cid:10)*(cid:14)%(cid:28)’<*=(cid:27)(cid:9))+(cid:26)(cid:28)(cid:27)(cid:9)%(*/9 (cid:26)*(cid:10)(cid:10)%(cid:26)+(cid:9))(cid:20)<<(cid:28)’(cid:28)(cid:9) 8(cid:28)+)8%*(cid:9)%’(cid:10)(%((cid:20)((cid:28)(cid:9)+0(cid:9)((cid:28)(cid:29)1’+/+89(cid:27)(cid:9)*(/*’(*(cid:27)(cid:9)(cid:20)(cid:10)* This volume contains 175 illustrations This work is subject to copyright. All rights are reserved, whether the whole or part of the material is concerned (cid:23)(cid:21)(cid:3)(cid:11)(cid:19)(cid:18)(cid:11)(cid:7)(cid:17)(cid:17)$(cid:9)(cid:24)(cid:6)(cid:16)(cid:23)(cid:3)(cid:9)(cid:16)(cid:25)(cid:9)(cid:24)(cid:4)(cid:7)(cid:5)(cid:23)(cid:17)(cid:7)(cid:24)(cid:19)(cid:16)(cid:5)(cid:27)(cid:9)(cid:4)(cid:3)(cid:21)(cid:4)(cid:19)(cid:5)(cid:24)(cid:19)(cid:5)(cid:22)(cid:27)(cid:9)(cid:4)(cid:3)(cid:13)(cid:15)(cid:23)(cid:3)(cid:9)(cid:16)(cid:25)(cid:9)(cid:19)(cid:17)(cid:17)(cid:15)(cid:23)(cid:24)(cid:4)(cid:7)(cid:24)(cid:19)(cid:16)(cid:5)(cid:23)(cid:27) broadcasting, reproduction by photocopying machine or similar means, and storage in data banks. © 2012 by CISM, Udine SPIN 86122731 All contributions have been typeset by the authors. %(cid:10)(cid:2)’(cid:9)OQV(cid:13)X(cid:13)Q5OY(cid:13)YX5V(cid:13)5(cid:9)(cid:10)(cid:21)(cid:4)(cid:19)(cid:5)(cid:22)(cid:3)(cid:4)6(cid:19)(cid:3)(cid:5)’(cid:3)!9(cid:16)(cid:4)(cid:31) PREFACE Periodicstructuralconfigurationsareubiquitous: manyheterogeneous structures and materials, both man-made and naturally occurring, feature geometry, micro-structural and/or materials properties that varyperiodicallyinspace. Theclassesofperiodicmaterialsandstruc- tures span a wide range of length scales, and a broad range of applica- tions. Periodic trusses, periodically stiffened plates, shells and beam- like assemblies can be found for example in many civil, aerospace, mechanical and ship constructions. Their introduction is mostly mo- tivated by structural strength and weight requirements, however recent studies have shown how the periodicity can be exploited to attenuate, isolate and localize vibrations. Such studies explore the unique ability of periodic assemblies to impede the propagation of elastic waves over specified frequency bands, within which strong attenuation of vibra- tion and radiated noise can be achieved. The attenuation levels that can be obtained through tailored structural periodicity far exceed the performance of most energy dissipation and damping mechanisms. For this reason, passive, active and hybrid periodic structural con- figurations are being proposed for the reduction of vibration trans- mission and structure-born as well as airborne noise. In addition, the understanding of the dynamics of periodic structures is essential for the analysis of bladed disc assemblies which are found in turbo machinery and in turbines for energy generation where failure mech- anisms due to localization phenomena may occur. At much smaller scales, extensive research is being devoted to the analysis and design of phononic metamaterials for a variety of applications. Phononic metamaterials are essentially periodic structural configurations ob- tained through composite designs featuring periodic modulations of mass and stiffness properties, or elastic lattice structures. Gigahertz communication devices, such as mobile phones, use phononic-based systems for their low-power filtering characteristics. Many sensing devices based on resonators, acoustic logic ports, and surface acous- tic wave-based filters rely on the unique band gap characteristics of periodic phononic materials. These properties are associated with the destructive and constructive interference of acoustic waves orig- inating at the periodic interfaces, which produce frequency band of strong attenuation of acoustic waves (band gaps). Depending on the inclusions, geometry, and elastic properties, one can design for spe- cific band gaps. In photonic crystals, periodic modulations of the dielectric properties of a medium allow guiding, focusing and steer- ing of electromagnetic waves. Properties modulations and engineered anisotropy in heterogeneous media can also produce negative refrac- tive indexes, both in photonics as well as in phononic metamaterials, which lead to super-lensing or super-focusing characteristics. Disper- sion of waves in media with boundaries or built-in micro-structure is a fundamental phenomenon, which occurs in problems of acous- tics, models of water waves, simple systems involving onedimensional harmonic oscillators, as well as complex elastic systems. Moreover, enhanced transmission based on formation of defect modes within an interface plays a crucial role in a wide range of practical applications involving filtering and polarisation of waves of different physical ori- gins. Other potential implications of the acoustic wave guiding tech- nology include active sensing of structural integrity, smart sensing of environment, dissipation of high frequency modes of vibration to enhance vehicle performance or stealth, as well as applications to the medical field for sensing or diagnostic applications. Complex dynam- ical phenomena may be encountered in nonlinear periodic media such as the existence of energy- depended nonlinear propagation regions. Depending on substructure coupling, distinctly nonlinear dynamical phenomena can arise, such as wave localization and solitary waves. Potential applications of such phenomena are currently investigated in the MEMS context, where arrays of coupled micro/nanoresonators have been recently proposed. The CISM course ”Wave propagation in linear and nonlinear periodic media: analysis and applications” was an opportunity to combine the material issued from such a vari- ety of applications aiming to present both the theoretical background and an overview of the state-of-the art in wave propagation in lin- ear and nonlinear periodic media in a consistent lecture format. The course is intended for doctoral and postdoctoral researchers in civil and mechanical engineering, applied mathematics and physics, aca- demic and industrial researchers, which are interested in conducting research in the topic. The opening chapter, by A.B. Movchan, M. Brun and N.V. Movchan, gives an overview of some mathematical models of wave propagation in structured media, with the emphasis on dispersion and enhanced transmission through structured interfaces. Chapter 2, by L. Airoldi, M. Senesi and M. Ruzzene, presents two examples of internally resonating metamaterials whose behavior is based on multi-field coupling. The first part of the chapter is devoted to the analysis of a one-dimensional waveguide with a periodic array of shunted piezoelectric patches. The second part presents the study of piezoelectric superlattices as an additional example of an internally resonant metamaterial. Topology optimization relevant to problems in vibration and wave propagation is then addressed in Chapter 3 by J. S. Jensen; in this chapter the steady-state optimization procedure for dynamical systems is extended to a nonlinear wave propagation problem and then the topology optimization procedure is applied to transient dynamic simulations for which the optimized material dis- tributions may vary in time. In Chapter 4, by F. Romeo, the dynamic behaviourofcontinuousanddiscretemodelsofbothlinearandnonlin- ear periodic mechanical systems are dealt with by means of maps. At first, linear problems consisting of general multi-coupled periodic sys- tems are presented and they are handled with linear maps, namely the transfer matrices of single units. Afterwards, a perturbation method is applied to the transfer matrix of a chain of continuous nonlinear beams while nonlinear maps are considered to address chains of non- linear oscillators. In the closing chapter, by A. Vakakis, analytical methodologies for analyzing waves in weakly or strongly nonlinear pe- riodic media are discussed. The generation of spatial chaos in ordered granular media, which are a special class of spatially periodic, highly discontinuous and strongly nonlinear media is eventually highlighted. CONTENTS Waves and Defect Modes in Structured Media by A.B. Movchan, M. Brun, N.V. Movchan.............. 1 Piezoelectric Superlattices and Shunted Periodic Arrays as Tunable Periodic Structures and Metamaterials by L. Airoldi, M. Senesi and M. Ruzzene................. 33 Topology Optimization by J.S. Jensen........................................... 109 Map-based Approaches for Periodic Structures by F. Romeo............................................. 161 Methodologies for Nonlinear Periodic Media by A. Vakakis............................................ 257 Waves and defect modes in structured media A.B. Movchana, M. Brunb, N.V. Movchana a DepartmentofMathematical Sciences, UniversityofLiverpool,LiverpoolL697ZL,U.K. b DepartmentofStructural Engineering, UniversityofCagliari,CagliariI-09123,Italy Abstract. Thepapergivesanoverviewofsomemathematical modelsofwavepropagationinstructuredmedia,withtheemphasis on dispersion and enhanced transmission through structured inter- faces. We begin with conventional definitions and classical models of dispersive waves, discuss lattice approximations and then show the results of the recent work on modelling of waves interacting with a structured stack acting as a polarizer of elastic waves. Spe- cial attention is given to the resonance modes which may enhance transmission across the structured stack. The analytical work is accompanied bynumerical simulations. 0.1 Introduction Dispersionofwavesinperiodicinhomogeneousmediaisimportantin many problems of physics, mechanics and engineering. A special mention shouldbegiventotheoreticalandexperimentalstudiesofphotonicbandgap materials (see, for example, Yablonovitch (1987, 1993)). Scalar models for BlochwavesinperiodiclatticesarediscussedinBrillouin(1953),Maradudin et al. (1963) and Kunin (1975). This theory naturally extends to vector problems of elasticity. In particular, dispersion of elastic waves in lattice systems of different types has been analysed in Martinsson and Movchan (2003), Jensen (2003), Cai et al. (2005). DynamiclatticeGreen’sfunctionsinthepropagatingfrequencyrange were analysed in Martin (2006), whereas the stop band Green’s functions and exponentially localised “defect modes” were studied in Movchan & Slepyan (2007). In wavepropagationproblems for structuredmedia, the classicalho- mogenisationapproacheshavelimitationswhenthewavelengthiscompara- blewiththecharacteristicsizeofelementsofthestructure,suchasatypical 2 A.B. Movchan, M. Brun, N.V. Movchan size of the elementary cell. In particular, this appears to be important in theanalysisofwaveinteractionwithfinitewidthstructuredinterfaces. Sev- eral classes of non-local structured interfaces were analysed in Bigoni and Movchan (2002) in static and dynamic configurations, which also included semi-discrete systems incorporating both continuous parts and a lattice. Brunetal. (2010a)haveaddressedanomaliesintransmissionofslowwaves through dynamic structured interface of finite width. Brun et al. (2010b) addressed the case of a shear-type structured interface excited by a plane pressure wave at an oblique incidence, and this paper also shows that the shear-type interface could serve as a polariser. In the present paper we aim to discuss the dispersion, polarisation and filtering of waves from a common perspective, with the emphasis on the dynamicsofstructuredinterfacesandconnectionsbetweendiscreteand high-contrast continuous systems. The structure of the paper is as follows. We begin with the discussion of the fundamental phenomena, such as wave dispersion, andinSection0.2we showaveryintuitive textbook exampleof dispersive waves,derived in the framework of the linear water wave theory. Section 0.3 includes the classical notion of Bloch-Floquet waves and an ex- plicitanalyticalstudyofwavedispersioninone-dimensionallatticesystems. Furthermore, this section also introduces the high-contrast continuous sys- tems, with the emphasis on the lattice approximations of the dispersion equations in such systems. An example of the transmission problem for a one-dimensionalfinitewidthstructuredinterfaceisdiscussedinSection0.5, where it is shown that an irregularity within the structure of the interface may lead to an enhanced transmission for waves of certain frequency. A full vector problem of elasticity is described in Section 0.6 for plane elastic wavesinteractingwithashear-typestructuredinterface;thefinitewidthin- terface contains severalparallelelastic bars,whosemotionis preferentialin the directionalong the interface. This creates aneffect ofpolarization,and we also describe an enhanced transmissionfor waves of certain frequencies. 0.2 Wave dispersion Thisintroductorysectiondiscussessomeclassicalexamplesofdisper- sivewaves,i.e. thewaveswhosespeedsaredifferentfordifferentfrequencies. Here we refer to the linear water wave theory, which is very well known in linearlisedmodelsoffluidflow(see,forexample,Billingham&King(2001), Ockendon et al. (2003)). The second example, included in Section 0.3, is a one-dimensional lattice system, known from classical texts (see, for ex- ample, Kittel (1996) and Brillouin (1953)). The dispersion relations are written in an explicit form, and formation of a stop band is discussed for

See more

The list of books you might like

Most books are stored in the elastic cloud where traffic is expensive. For this reason, we have a limit on daily download.