Sonic Crystals: Fundamentals, characterization and experimental techniques

Transcription

1 Sonic Crystals: Fundamentals, characterization and experimental techniques A. C e b r e c o s 1 L a u m, L e M a n s U n i v e r s i t é, C N R S, A v. O. M e s s i a e n, , L e M a n s Collaborators in t h is work: L A U M : J. P. G r o b y, V. R o m e r o - García U P V: N. J i m é n e z, V. S á n c h e z - M o r c i l l o, L. M. G a r c í a - R a f f i U C B : M. H u s s e i n, D. K r a t t i g e r

2 Outline Part I Introduction to Sonic Crystals Origins and fundamentals Bandgaps. Dispersion relation. Group and phase velocities. Dispersion. EFC Methods for Dispersion Relation calculation Plane Wave expansion Finite-elements for band structure calculation in time-domain Part II Experimental techniques for the characterization of Sonic Crystals Dispersion relation using Space-time to frequency-wavevector transformation Methodology 2D Experimental relation using SLatCow Deconvolution method for analysis of reflected fields by SCs Methodology Practical application: Sonic Crystals for noise reduction at the launch pad EXPERIMENTAL TECHNIQUES FOR THE CHARACTERIZATION OF SONIC CRYSTALS 2

3 Definition and origins General definition: (Solid state physics) A crystal is a solid material whose constituents, such as atoms, molecules or ions, are arranged in a highly ordered microscopic structure, forming a lattice that extends in all directions Artificial (or even natural) materials whose physical properties are periodic functions of the space (1D, 2D, 3D) Optical properties (electromagnetic waves) Dielectric constant (refractive index) Photonic crystal E. Yablonovitch. PRL, 58, 2059, (1987). Engineer photonic density of states to control the spontaneous emission of materials embedded in the photonic crystal. S. John. PRL, 58, 2486, (1987). Using photonic crystals to affect localisation and control of light. E. Yablonovitch et al. PRL, 67, 2295, (1991). Elastic properties (elastic and acoustic waves) Density and elastic constants (speed of sound) Phononic crystal Periodic distribution of solid scatterers in a solid host medium M. M. Sigalas and E. N. Economou. JSV. 158, 377. (1992) M. S. Kushwaha et al,. PRL, 71, (1993) Sonic crystal Particular case in which the host medium is a fluid. R. Martínez-Sala. Nature, (1995). M. S. Kushwaha. APL, 70, (1997) J. V. Sánchez-Pérez, PRL, 80, (1998) The study of photonic, phononic and sonic crystals makes use of the same concepts and theories developed in quantum mechanics for electron motion: Direct and reciprocal lattices, Brillouin zone, Bragg interferences, Bloch periodicity, band structures ORIGINS AND FUNDAMENTALS

4 Direct Space 2D Square lattice There is a unique one-dimensional (1D) periodic system. Five two-dimensional (2D). Fourteen three-dimensional (3D) different lattices Geometrical parameters Unit cell and lattice constant Filling fraction Scatterer shape ORIGINS AND FUNDAMENTALS

5 Reciprocal Space The reciprocal space (k-space) is used to study the wave propagation characteristics in periodic structures (Dispersion relation, bandgaps, propagation direction): ORIGINS AND FUNDAMENTALS

6 Reciprocal Space The study of the band structure can be limited to the Irreducible Brillouin zone. For the case of a square lattice the IBZ is reduced to a triangle. The scatterer should accomplish the same symmetries in the direct space ORIGINS AND FUNDAMENTALS

7 Direct and Reciprocal Space Direct space Reciprocal space Propagation pressure fields, Vibrational modes Band structures, Equifrequency contours, surfaces ORIGINS AND FUNDAMENTALS

8 Origins and interpretation of the band gaps: Bragg interferences Bragg interferences J. D. Joannopoulos (Photonic crystals: Molding the flow of light) Illustration of Evanescent behaviour, 1D E. Yablonovitch,. Scientific American, 285. (6). Dec. 2001, pp BANDGAPS. DISPERSION RELATION

9 Evidence of evanescent modes inside the BG Analytical, numerical and experimental results V. Romero-García et al,. Appl. Phys. Lett., 96, , (2010) V. Romero-García et al,. J. Appl. Phys. 108, , (2010) BANDGAPS. DISPERSION RELATION

10 Origins of the band gaps w(k) in homogeneous medium Plane wave propagating in a 1D homogeneous medium BANDGAPS. DISPERSION RELATION

11 Origins of the band gaps Periodicity in real space periodicity in reciprocal space Plane wave propagating in a 1D homogeneous medium BANDGAPS. DISPERSION RELATION

12 Origins of the band gaps Periodic w(k) repetitions of period 2pi/a (replicated bands due to periodicity) Plane wave propagating in a 1D homogeneous medium BANDGAPS. DISPERSION RELATION

13 Origins of the band gaps Periodic variation of the physical properties of the medium Plane wave propagating in a 1D periodic medium BANDGAPS. DISPERSION RELATION

14 Origins of the band gaps Creation of bandgaps and dispersion Plane wave propagating in a 1D periodic medium BANDGAPS. DISPERSION RELATION

15 Origins of the band gaps Band gap frequency and dependence of its width Plane wave propagating in a 1D periodic medium BANDGAPS. DISPERSION RELATION

16 2D Dispersion relation w(k) in 2D is now a surface Plane wave propagating in a 2D homogeneous medium BANDGAPS. DISPERSION RELATION

17 2D Dispersion relation Periodicity in x and y directions. Main directions of simmetry in reciprocal space Plane wave propagating in a 2D homogeneous medium BANDGAPS. DISPERSION RELATION

18 2D Dispersion relation Dispersion relation along the main simmetry points of the reciprocal space Plane wave propagating in a 2D homogeneous medium BANDGAPS. DISPERSION RELATION

19 2D dispersion relation Periodic variation of the physical properties. Creation of pseudo gaps for low ff Plane wave propagating in a 2D periodic medium BANDGAPS. DISPERSION RELATION

20 2D dispersión relation Increasing ff and/or impedance contrast will eventually create a full band gap Plane wave propagating in a 2D periodic medium BANDGAPS. DISPERSION RELATION

21 Phase and group velocities DISPERSION. GROUP AND PHASE VELOCITIES

22 Group velocity and phase velocity Negative group velocity: Certain frequencies in the second band Source: Institute of Sound and Vibration Research. University of Southampton DISPERSION. GROUP AND PHASE VELOCITIES

23 Group velocity and phase velocity Higher phase velocity: Dispersive part of first band Source: Institute of Sound and Vibration Research. University of Southampton DISPERSION. GROUP AND PHASE VELOCITIES

24 Group velocity and phase velocity Zero group velocity: Localized wave Source: Institute of Sound and Vibration Research. University of Southampton DISPERSION. GROUP AND PHASE VELOCITIES

25 Understanding dispersion Group velocity Phase velocity N = 200 layers Rigid boundary conditions Gaussian pulse at w n = 0.4 Plane wave propagating in a 1D periodic medium DISPERSION. GROUP AND PHASE VELOCITIES 25

26 Understanding dispersion Group velocity Phase velocity N = 200 layers Rigid boundary conditions Gaussian pulse at w n = 0.7 Plane wave propagating in a 1D periodic medium DISPERSION. GROUP AND PHASE VELOCITIES 26

27 Understanding dispersion Group velocity Phase velocity N = 200 layers Rigid boundary conditions Gaussian pulse at w n = 1 Plane wave propagating in a 1D periodic medium DISPERSION. GROUP AND PHASE VELOCITIES 27

28 Equifrequency contours DISPERSION. GROUP AND PHASE VELOCITIES

29 Methods for dispersion relation calculation Generally considering infinite media by applying periodic boundary conditions (Bloch theory) PERIODIC : INFINITE MEDIUM Transfer matrix method (TMM) Plane wave expansion (PWE) Multiple scattering method (MST) Finite element method (FEM) Finite difference in time domain(fdtd) Finite element in time domain (FETD) CHARACTERISTICS Dimensionality: 1D,2D,3D (TMM 1D, PWE, FEM, FDTD all, etc.) Handling different media (limitations in PWE solid-fluid except rigid inclusions in air or holes in solid matrix ) Handling geometry (structure factor in PWE, meshing in FEM or FDTD) Steady-state or time dependent METHODS FOR DISPERSION RELATION CALCULATION 29

30 PWE. Eigenvalue problem Plane wave expansion (PWE) Wave equation (inhomogeneous medium) Considering a periodic medium Fourier series expansion Bloch s theorem The solution of a wave equation with periodic potential can be written in the form: PLANE WAVE EXPANSION

31 PWE. Eigenvalue problem Model the shape of the scatterer: Structure factor Consider that the periodic structure is made of two materials, A and B, being B the host material Kushwaha et al., PRB, 49. (1994) Cylinder Square Other shapes Hexagonal, rectangular, elliptic V. Romero-García. JPD, (2013) R. Wang et al, JAP, 90, 2001 PLANE WAVE EXPANSION

32 PWE. Eigenvalue problem PLANE WAVE EXPANSION

33 Finite element method in time-domain Finite element in time-domain for elastic band structure calculation (FETD) Time-dependent Bloch periodicity Excitation required Continuum Equation of motion: A. Cebrecos et al. The finite-element method for elastic band structure calculation. Computer Physics Communications. Under review Strong form general elastodynamic problem Space Discretization FINITE-ELEMENTS FOR BAND STRUCTURE CALCULATION IN TIME-DOMAIN

34 Unit-cell finite-element model Weak form: Weighting and shape functions Direct stiffness method Element to global Option: Eigenvalue problem or time-integration (forced term) Bloch theory (BC s) FINITE-ELEMENTS FOR BAND STRUCTURE CALCULATION IN TIME-DOMAIN

35 Unit-cell time-domain simulation Time integration method: Center difference Newmark scheme (Explicit) Computationally efficient Less storage compared to implicit methods Conditionally stable CFL FINITE-ELEMENTS FOR BAND STRUCTURE CALCULATION IN TIME-DOMAIN

36 Unit-cell time-domain simulation Transient excitation Ricker wavelet Calculation of frequency band structure FINITE-ELEMENTS FOR BAND STRUCTURE CALCULATION IN TIME-DOMAIN

37 Unit-cell time-domain simulation Transient excitation Ricker wavelet Calculation of frequency band structure FINITE-ELEMENTS FOR BAND STRUCTURE CALCULATION IN TIME-DOMAIN

38 Numerical examples. Bloch Modeshapes FINITE-ELEMENTS FOR BAND STRUCTURE CALCULATION IN TIME-DOMAIN

39 Dispersion relation using Space-time to frequencywavevector transformation PART II 39

40 1D Dispersion relation recovery: Methodology Space-Time Fourier Transformation 1D periodic medium DISPERSION RELATION USING SPACE-TIME TO FREQUENCY-WAVEVECTOR TRANSFORMATION 40

41 1D Dispersion relation recovery Spatial sampling 1D periodic medium DISPERSION RELATION USING SPACE-TIME TO FREQUENCY-WAVEVECTOR TRANSFORMATION 41

42 1D Dispersion relation recovery What is the right spatial sampling measuring periodic structures? Using analogy from temporal signals: From Nyquist sampling theorem, considering periodicity in reciprocal space: Finally, consider a SC of a given length: Lattice constant N unit cells For smaller dx, greater N N UNIT CELLS DEFINES RESOLUTION in k-space DISPERSION RELATION USING SPACE-TIME TO FREQUENCY-WAVEVECTOR TRANSFORMATION 42

43 1D Dispersion relation recovery Influence of SC size, undersampling and oversampling space Number of Unit cells Undersampling Oversampling DISPERSION RELATION USING SPACE-TIME TO FREQUENCY-WAVEVECTOR TRANSFORMATION 43

44 2D Dispersion relation recovery: Methodology 2D Acoustic metamaterial Quarter-wave resonators as scatterers (Lossless) 50 x 50 unit cells 50 measurement points in center line Point source at the center Angular components in all directions Bands overlapping Dispersion relation incomplete! DISPERSION RELATION USING SPACE-TIME TO FREQUENCY-WAVEVECTOR TRANSFORMATION 44

45 2D Dispersion relation recovery: Methodology 2D Acoustic metamaterial Quarter-wave resonators as scatterers (Lossless) 50 x 50 unit cells 50 measurement points in center line Plane wave excitation New angular components created due to scattering Dispersion relation incomplete! DISPERSION RELATION USING SPACE-TIME TO FREQUENCY-WAVEVECTOR TRANSFORMATION 45

46 2D Dispersion relation recovery: Methodology Spatial filtering in the reciprocal space (k-space) 1. 1 measurement point per scatterer 2. Transformation to k-space (2D) Isofrequency contours 3. Selection of main symmetry directions for frequencies of interest DISPERSION RELATION USING SPACE-TIME TO FREQUENCY-WAVEVECTOR TRANSFORMATION 46

47 2D Dispersion relation recovery: Methodology Spatial filtering in the reciprocal space (k-space) Results using a point source DISPERSION RELATION USING SPACE-TIME TO FREQUENCY-WAVEVECTOR TRANSFORMATION 47

48 2D Dispersion relation recovery: Methodology Spatial filtering in the reciprocal space (k-space) Results using a plane wave DISPERSION RELATION USING SPACE-TIME TO FREQUENCY-WAVEVECTOR TRANSFORMATION 48

49 Experimental dispersion relation measurement SLaTCow method: Complex dispersion relation A. Geslain et al., J. Appl. Phys. 120,135107, (2016) Wednesday morning at SAPEM Analysis for every frequency Set of parameters defining theoretically the propagatio: amplitude, phase, real and imaginary part of the wave vector Optimization minimizing the difference between and DISPERSION RELATION USING SPACE-TIME TO FREQUENCY-WAVEVECTOR TRANSFORMATION 49

50 Experimental dispersion relation measurement SLaTCow method: Complex dispersion relation Analysis for every frequency Set of parameters defining theoretically the propagatio: amplitude, phase, real and imaginary part of the wave vector Optimization minimizing the difference between and DISPERSION RELATION USING SPACE-TIME TO FREQUENCY-WAVEVECTOR TRANSFORMATION 50

51 Experimental dispersion relation 24 x 4 unit cells 1 measurement point per scatterer Numerical results Experiments DISPERSION RELATION USING SPACE-TIME TO FREQUENCY-WAVEVECTOR TRANSFORMATION 51

52 Experimental dispersion relation 24 x 4 unit cells 1 measurement point per scatterer DISPERSION RELATION USING SPACE-TIME TO FREQUENCY-WAVEVECTOR TRANSFORMATION 52

53 Experimental dispersion relation 24 x 4 unit cells 1 measurement point per scatterer DISPERSION RELATION USING SPACE-TIME TO FREQUENCY-WAVEVECTOR TRANSFORMATION 53

54 Deconvolution method for analysis of reflected fields by SCs PART II 54

55 Experimental evaluation of a SC Impulse Response Context of the problem: Study feasibility of Sonic Crystals in reducing impact of the backward reflected field emitted by a sound source in a simplified scaled model of a launch pad (Proof of concept) Requisites (Greatly simplified problem): Linear regime Static source Broadband frequency study Scaled model in water (ultrasonic regime) Challenge: Analysis of reflected field by a SC Insertion loss in reflection Diffusion coefficient ESA ITI Type A project: Sonic Crystals for Noise Reduction at the Launch Pad DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS

56 Experimental evaluation of a SC Impulse Response Context of the problem: Study feasibility of Sonic Crystals in reducing impact of the backward reflected field emitted by a sound source in a simplified scaled model of a launch pad (Proof of concept) Requisites: Linear regime Static source Broadband frequency study Scaled model in water (ultrasonic regime) Challenge: Analysis of reflected field by a SC Insertion loss in reflection Diffusion coefficient Areas of interest Sound source Reflector: Sonic crystal Rigid reflector Ground surface ESA ITI Type A project: Sonic Crystals for Noise Reduction at the Launch Pad DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS

57 Linear and time invariant system: Theory Transfer function H(f): Widely used in experiments using SC s Calculation of reflection, transmission and absorption coefficients Insertion Loss in attenuation devices DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS

58 Linear and time invariant system: Theory Impulse response h(t): Room acoustics: Acoustic quality parameters Weakly nonlinear system identification Incident and reflected pressure field Farina A, Fausti P. Journal of Sound and Vibration 2000;232(1): A. Novak, et al., IEEE Transactions on. Vol. 63(8), pp (2014) Farina, A. Audio Engineering Society Convention 108. Audio Engineering Society, DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS

59 Impulse response deconvolution: Practical example Input signal: Logarithmic sine sweep: Quasi-ideal case 1: DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS

60 Impulse response deconvolution: Practical example Input signal: Logarithmic Sine sweep: Quasi-ideal case 2: DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS

61 Experimental setup Signal parameters Computer. Labview for measurement control 3D Motorized axis Hydrophone Piezoelectric transducer DAQ-PXI Digital Signal Generator Digital oscilloscope RF Amplifier DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS

62 Impulse response deconvolution: Example Input signal: Logarithmic Sine sweep: Real case: System response + reflections DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS

63 Impulse response deconvolution: Example Input signal: Logarithmic Sine sweep: Real case: System response + reflections DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS

64 Samples used in the experiments Characteristics of the SCs Four different samples (2D SCs) Square shape scatterers Square and triangular lattice Low and filling fraction 3D Printed Selective laser melting DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS

65 Incident and reflected field separation Experimental results: Incident field f = 350 khz First Band f = 500 khz Band Gap f = 700 khz Second Band DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS

66 Incident and reflected field separation Reflected field. Square lattice High filling fraction f = 350 khz Low Band f = 500 khz Band Gap f = 700 khz High Band DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS

67 Experimental wave propagation. Convolution signal on demand Input: Sinusoidal pulse (Narrow bandwidth, band gap) DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS 67

68 Experimental wave propagation Input: Sinusoidal pulse (Narrow bandwidth, 2 Band) DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS 68

69 Insertion loss results Modified Insertion loss to study reflection IL along the space integrated in frequency Reduction of the reflected field depending on the reflection angle DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS 69

70 Insertion loss results Modified Insertion Loss to study reflection IL in frequency bands integrated in ROI Reduction of the reflected field due to diffusion Higher in propagative bands Lower in the BG DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS 70

71 Difussion coefficient Near to far field transformation Projection of the pressure in near to field to infinity Esentially it is a spatial Fourier transform Angular information Reflection from a flat rigid surface T. J. Cox, P. D'antonio. Acoustic absorbers and diffusers: theory, design and application. Crc Press, DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS 71

72 Difussion coefficient Diffusion coefficient Normalized diffussion coeficient Quantification of the type of reflection Specular Diffuse ISO :2012 Acoustics -- Sound-scattering properties of surfaces -- Part 2: Measurement of the directional diffusion coefficient in a free field DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS 72

73 Difussion coefficient results Far field results Normalized diffussion coeficient Normalized diffussion coeficient Quantification of the type of reflection Specular Diffuse DECONVOLUTION METHOD FOR ANALYSIS OF REFLECTED FIELDS BY SCS 73

74 Sonic Crystals: Fundamentals, characterization and experimental techniques A. C e b r e c o s 1 L a u m, L e M a n s U n i v e r s i t é, C N R S, A v. O. M e s s i a e n, , L e M a n s Collaborators in t h is work: L A U M : J. P. G r o b y, V. R o m e r o - García U P V: N. J i m é n e z, V. S á n c h e z - M o r c i l l o, L. M. G a r c í a - R a f f i U C B : M. H u s s e i n, D. K r a t t i g e r

75 Positive, zero and negative diffraction. Focusing of waves using finite SC s: Curvature of the wave front Character of the incident wave Plane wave Point source Sound beam (Gaussian beam) Width of the source D=2a D=8a DISPERSION. GROUP AND PHASE VELOCITIES

76 Isofrequency contours & Focusing regimes Focusing of waves using finite SC s: Interplay between beam and periodic media Band structure and Isofrequency contours (PWE) Band structure a = 5,25 mm r = 0,8 mm Isofrequenc y contour Spatial spectrum of the incident beam D=2 a D=8a Source angular spectrum Extended BZ DISPERSION. GROUP AND PHASE VELOCITIES

77 Results Spatial dispersion completely parabolic D=8a Accumulated phase shift D=2a Focusing distance DISPERSION. GROUP AND PHASE VELOCITIES