2008
DOI: 10.1109/tuffc.929
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Iterative high-resolution wavenumber inversion applied to broadband acoustic data

Abstract: This paper presents the results of an iterative high-resolution wavenumber inversion algorithm applied to acoustic waveguides in which wave propagation is described by propagating modes. Following work on the first description of the inversion algorithm, a generalization to broadband signals is performed and experimental data are investigated. The algorithm leads to dispersion curves for propagating modes in the case of an ultrasonic waveguide and an elastic plate. Results are compared with spatial-temporal Fo… Show more

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Cited by 14 publications
(4 citation statements)
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“…Periodic structures or locally resonant systems, also known as metamaterials, have revolutionized the control of waves these last years [1,2]. The main physical properties of these structured media, as for example the opening of band gaps [3,4], the slow wave frequency band [5,6], or the spatial filtering [7], among others, can be directly derived from the complex dispersion relation [8][9][10][11][12]. In addition to dispersive effects, wave attenuation can be caused by factors such as geometric attenuation or intrinsic material loss (e.g., heat or viscous dissipation).…”
Section: Introductionmentioning
confidence: 99%
“…Periodic structures or locally resonant systems, also known as metamaterials, have revolutionized the control of waves these last years [1,2]. The main physical properties of these structured media, as for example the opening of band gaps [3,4], the slow wave frequency band [5,6], or the spatial filtering [7], among others, can be directly derived from the complex dispersion relation [8][9][10][11][12]. In addition to dispersive effects, wave attenuation can be caused by factors such as geometric attenuation or intrinsic material loss (e.g., heat or viscous dissipation).…”
Section: Introductionmentioning
confidence: 99%
“…4,7,8 The dispersion of waves propagating through materials is typically interpreted in the context of frequency and wavenumber domain information and obtained from discrete spatiotemporal data via discrete Fourier transforms and related methods. [9][10][11][12][13][14] However, such techniques typically only supply real wavenumber information (or their magnitudes) from twodimensional, discrete, spatiotemporal wave propagation information, such as may be obtained from scanned receiver measurements. Several methods have been proposed to characterize wave attenuation and extract complex wavenumber information; [15][16][17][18][19][20][21][22] however, each has restrictions, as: (i) they are usually based on measurements of wave amplitude decrease with respect to time, [15][16][17][18] (ii) they are iterative methods applied in space, like the modified Prony method, 19 (iii) the number of modes has to be known in advance or a unique mode has to be isolated, [15][16][17]20,21,23 (iv) the modes contributing significantly to the signal are presumed to not interact or overlap with one another, or (v) they must include a third dimension of information, such as would be the case in an experiment with a scanned emitter and a receiver.…”
Section: Introductionmentioning
confidence: 99%
“…Des méthodes à hautes résolutions (HR) sont souvent préférées pour surmonter ces limites (Marcos, 1998). Les modèles autorégressifs (Shang et al, 1988 ;Becker, Frisk, 2006 ;Philippe et al, 2008 ;Le Courtois, Bonnel, 2014a) et les méthodes en sousespace comme MUSIC, ESPRIT (Rajan, Bhatta, 1993) et les Matrix Pencil (Lu et al, 1998, ont montré leur intérêt pour l'estimation des k rm . Cependant, si ces méthodes améliorent la résolution, elles restent sujettes à une plus grande sensibilité au bruit.…”
Section: Introductionunclassified