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Cylindrical coordinates of the hollow cylinder and dimensions. 

Cylindrical coordinates of the hollow cylinder and dimensions. 

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Guided time-harmonic shear horizontal SH waves propagating in the circumferential direction of an isotropic hollow cylinder are studied. The dispersion equation as well as the displacement and stress field across the wall thickness is derived analytically. Compared with the SH waves in a plate, a quantitative guideline of how well a plate model can...

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... cracks and corrosion defects are often found in both industrial and military hollow cylindrical structures like pipelines and cylindrical containers. Reliable and easy-to-use inspection systems are in great need to locate the defects and to be able to characterize and size them efficiently. Hirao and Ogi 1 proposed a circumferential SH-wave Electromagnetic Acoustic Transducer ͑ EMAT ͒ technique for detecting corrosion defects on the outer surface of steel pipelines with and without protective resin coating. Gauthier 2 used multimode SH waves generated by EMATs to form B-scan images of a defect on a pipe. The reflection and transmission coefficients of SH waves passing through a two-dimensional surface- breaking defect or a stringer-like internal inclusion in a pipe was reported by the present authors. 3 However, all of these publications were based on an empirical plate-model approximation for a pipe of large diameter-to-wall-thickness ratio. A rigorous theory of guided SH waves propagating in the circumferential direction of a hollow cylinder needs to be established. 4 Gazis 5,6 theoretically investigated guided waves that propagate in the axial direction and are resonant in the circumferential direction of a hollow cylinder. The case when the axial wave number is zero decouples into axially motion- independent plane–strain vibration and longitudinal shear vibration, both of which are standing waves in the circumferential direction. Liu and Qu 7 developed the model of guided plain–strain waves propagating in the circumferential direction of a hollow cylinder, with emphasis on the dispersion relation and displacement profile derivation and discussion. In this paper, the guided time-harmonic SH wave propagating in the circumferential direction of a hollow cylinder is studied. The dispersion equation as well as the displacement and stress distribution across the wall of the hollow cylinder is derived analytically. They are compared with that of the SH waves in a plate of the same thickness numerically. Rela- tive errors of the phase and group velocities when using a plate model to approximate a pipe are given as a quantitative measure of whether that approximation is valid. With the approximated plate model, the guided wave interaction and scattering from a three-dimensional defect in a hollow cylindrical structure of large diameter-to-wall-thickness ratio could be tackled without extensive eigenmode and wave structure calculations in each scattering direction. 8 Consider steady-state time-harmonic waves propagating in the circumferential direction of a hollow cylinder of inner radius a and outer radius b , as shown in Fig. 1. Assume the material is linearly elastic and isotropic, and the wave motion is independent of z . Two types of guided waves are possible in this hollow cylinder: one is the plane–strain vibration wave similar to the Lamb wave in a plate; 7 the other is the longitudinal shear wave, which will be studied in detail in this paper. The analytical derivation of the frequency equation of the guided circumferential SH waves begins with Navier’s equation of motion as Eq. ͑ 1 ͒ , where u is the displacement vector, ␳ is the density, ␭ and ␮ are Lam ́ ’s constants, respectively ␮ ٌ 2 u ϩ ͑ ␭ ϩ ␮ ͒ ٌٌ • u ϭ ␳ ͑ ץ 2 u / ץ t 2 ͒ . ͑ 1 ͒ Consider only the displacement in the z direction in the cylindrical coordinates, i.e., u r ϭ u ␪ ϭ 0 and u z 0; Eq. ͑ 1 ͒ can be written ...

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Citations

... This analytical expression is consistent with the SH wave dispersion equation for a plate. [22] It should be noted that the pipe-to-plate approximation is reasonable only when the thickness to outer diameter ratio of the pipe, i.e., the standard dimension ratio (SDR), is less than 10%-15%. [23] 3. Inversion formulas for thickness ...
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... hollow cylinders the wave equation of which were given by Liu [22] and Zhao [23], respectively. Dispersion and multimodality are key characteristics of wave propagation in pipelines, governed by the frequency-dependent nature of guided waves in waveguides. ...
... Monitoring of mechanical changes due to pitting, cracking, material conversion from corrosion and/or erosion, and material addition from material migration and accumulation in pipes, especially in hard-to-access environments [1], such as under insulation or paint, is important in many industries that involve liquid or gas storage and flow [2,3]. Commercialguided wave systems show a sensitivity to changes of 5% or above of cross-sections [4,5]. ...
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... Circumferential guided-wave-based method is especially suitable for monitoring large-diameter pipes such as pressure vessels and oil tanks, while for long range pipes, it can be used to inspect the risk areas such as the welding zones and pipe support regions. Among the circumferential guided wave modes in pipes, the fundamental circumferential shear horizontal (CSH0) wave is an appealing wave mode to develop phased array systems, since it is quasi-nondispersive [35]. However, there appears no attempt to develop a CSH0 wave phased array, which is mainly attributed to the difficulty of generating pure CSH0 wave. ...
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... where p is the angular wavenumber with respect to the propagation direction, θ, ω is the angular frequency, n is the mode order, A n is the amplitude of each mode, and U n is the displacement profile along the r-coordinate for each mode. The exact dispersion relationship and mode-profile for CSH waves depend on the pipe's thickness and outer to inner radius ratio [13].The propagation of CSH guided waves is more complex than in the plate, due to its solutions containing Bessel functions. The proof for these solutions will not be presented in this work in detail and can be found in the literature [7], [12], [13], but in general the characteristic equation for a single layer annulus is given the frequencywavenumber pairs that nullify the determinant of the following matrix: ...
... The exact dispersion relationship and mode-profile for CSH waves depend on the pipe's thickness and outer to inner radius ratio [13].The propagation of CSH guided waves is more complex than in the plate, due to its solutions containing Bessel functions. The proof for these solutions will not be presented in this work in detail and can be found in the literature [7], [12], [13], but in general the characteristic equation for a single layer annulus is given the frequencywavenumber pairs that nullify the determinant of the following matrix: ...
... In spite of difficulties in generating the SH wave [11], theoretical studies and SH guided wave applications have received increasing interest. Various analytical and numerical studies about the characteristics of SH guided waves have been reported [12][13][14][15][16], and most of them search for numerical solutions. Based on the Peano-series method, a theoretical formulation for shear-horizontal waves in the PZT-5H piezoelectric plate has been presented [17]. ...
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... Guided circumferential waves, which can be effectively used to detect and characterize structural defects or fatigue cracks in cylindrical structures, have been an active research topic because of their pivotal significance not only in NDE (Valle et al., 2001;Luo et al., 2005) but also in the application realm of EA devices (White, 1970). For isotropic linear elastic materials, the investigation of Lamb-type or SH-type circumferential waves (hereafter abbreviated as Lamb waves or SH waves) propagating along the cylindrical surface have been conducted by Liu and Qu (1998), Gridin et al. (2003), and Zhao and Rose (2004), just to name a few. The guided circumferential waves propagating in anisotropic cylindrical curved plates were studied numerically by the Fourier series expansion technique (Towfighi et al., 2002). ...
... Since guided circumferential waves can be readily utilized to detect and characterize structural defects or fatigue damages in cylindrical structures (Liu and Qu, 1998;Valle et al., 2001;Zhao and Rose, 2004;Luo et al., 2005), in this section, we will consider a small-amplitude circumferential wave motion in an EA tube subjected to the biasing fields determined in Section 3. Based on the state-space formalism obtained in the previous section, the approximate laminate technique will be used here to derive the dispersion relations of the circumferential waves. ...
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... Viktorov [54] first studied the problem of wave propagation in cylindrical layers and showed that waves propagation in the circumferential direction of cylindrical structures are quite different from those propagation in planar structures. Qu and his collaborators [55,56] presented detailed derivations of the dispersion equations and wave structures of CLamb waves, while the problem of CSH waves propagation in cylindrical structures was firstly addressed by Zhao and Rose [48]. ...
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Shear horizontal (SH) waves are of great importance in structural health monitoring (SHM) and nondestructive testing (NDT), since the lowest order SH wave in isotropic plates is non-dispersive. The SH waves in plates, circumferential SH waves and torsional waves in pipes have remarkable resemblances in dispersion characteristics and wave structures, so the latter two can also be called as SH waves in pipes. This paper reviews the state-of-the-art research on SH wave transducers for SHM and NDT. These transducers are grouped into the following categories: Lorentz-force-based electromagnetic acoustic transducers (EMATs), magnetostrictive EMATs, shear wave piezoelectric wedge transducers, thickness-shear piezoelectric transducers and face-shear piezoelectric transducers. The working principles, applications, merits and limitations of different kinds of SH wave transducers are summarized, with a focus on discussing the various configurations for exciting and receiving directional, omnidirectional SH waves in plates and torsional waves in pipes. This paper is expected to greatly promote the applications of SH waves in SHM, NDT and the related areas such as elastic metamaterials.
... Liu et al. presented the first numerical examples of the dispersion curves for circumferential Lamb waves propagating in the isotropic circular annulus [3]. A nearly decade later, the first results for the circumferential SH waves were introduced in the reference [5,6]. In the above study, they use Bessel functions to expand the displacement field. ...
... They all asymptotically approach the Rayleigh wave velocity, which is nondispersive. These characteristics much resemble the circumferential SH modes in the isotropic hollow cylinder [6]. ...
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The fundamental circumferential shear horizontal (CSH0) wave is of practical importance in monitoring corrosion defects in large-diameter pipes due to its virtually non-dispersive characteristics. However, so far, there have been limited CSH0 wave transducers which can be used to constitute a structural health monitoring (SHM) system for pipes. Moreover, the CSH0 wave’s capability of sizing the corrosion-like defect has not yet been confirmed by experiments. In this work, firstly, the mechanism of exciting CSH waves was analyzed. A method based on our previously developed bidirectional SH wave piezoelectric transducers was then proposed to excite the pure CSH0 mode and first order circumferential shear horizontal (CSH1) mode. Both finite element simulations and experiments show that the bidirectional transducer is capable of exciting pure CSH0 mode traveling in both circumferential directions of a 1 - mm thick steel pipe from 100 to 300 kHz. Moreover, this transducer can also serve a sensor to detect CSH0 mode only by filtering circumferential Lamb waves over a wide frequency range from 100 to 450 kHz. After that, a method of sizing a rectangular notch defect by using CSH0 wave was proposed. Experiments on an 11 - mm thick steel pipe show that the depth and circumferential extent of a notch can be accurately determined by using the proposed method. Finally, experiments were performed to investigate the reflection and transmission characteristics of CSH0 and CSH1 waves from notches with different depths. It was found that transmission coefficients of CSH0 mode decrease with the increasing of notch depth, which indicates that it is possible to monitor the depth change of corrosion defects by using CSH0 wave.