2016
DOI: 10.1016/j.mechrescom.2016.03.007
|View full text |Cite
|
Sign up to set email alerts
|

Investigation of guided waves propagation in orthotropic viscoelastic carbon–epoxy plate by Legendre polynomial method

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

0
36
0

Year Published

2017
2017
2022
2022

Publication Types

Select...
7
1

Relationship

1
7

Authors

Journals

citations
Cited by 35 publications
(50 citation statements)
references
References 12 publications
0
36
0
Order By: Relevance
“…, and H j m are the corresponding elements of these matrices, which can be obtained by equation (8) Note that in equation (11), once we specify a fixed value of v, it does not have the structure of a general eigenvalue problem in k. In previous research works, 12,13 equation (11) was transformed into an eigenvalue problem with eigenvalue v. For a propagating wave, it is simple to specify real k and then solve for v. But for an evanescent wave, it is useless because the wavenumber is complex, which involves a multivariable search. To deal with this problem, we develop a new solution procedure to recast the equation again in the form of a general eigenvalue problem, as shown below.…”
Section: Mathematics and Formulation Of The Problemmentioning
confidence: 99%
See 1 more Smart Citation
“…, and H j m are the corresponding elements of these matrices, which can be obtained by equation (8) Note that in equation (11), once we specify a fixed value of v, it does not have the structure of a general eigenvalue problem in k. In previous research works, 12,13 equation (11) was transformed into an eigenvalue problem with eigenvalue v. For a propagating wave, it is simple to specify real k and then solve for v. But for an evanescent wave, it is useless because the wavenumber is complex, which involves a multivariable search. To deal with this problem, we develop a new solution procedure to recast the equation again in the form of a general eigenvalue problem, as shown below.…”
Section: Mathematics and Formulation Of The Problemmentioning
confidence: 99%
“…7 There are also many methods taking FGM as a continuous gradient medium to be proposed for analyzing guided waves in FGM structures, such as the Wentzel-Kramers-Brillouin method, 8 power series method, 9 reverberation-ray matrix method, 10 state vector method, 11 and orthogonal polynomial series method. 12,13 Such methods have been successfully applied to computing, two-dimensional (2D), and less often three-dimensional (3D), dispersion curves for guided waves. Recently, the guided waves in nanostructures and functionally graded nanostructures have also been extensively investigated.…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, although the Legendre polynomial method is quite versatile for guided wave problems, it involves a large amount of numerical integration calculations, resulting in a low computational efficiency. [29][30][31][32][33][34] This paper presents a recursive Legendre polynomial analytical integral (RLPAI) method to determine complete roots of the dispersion equation of guided waves in a rectangular orthotropic composite bar. The RLPAI method does not require the large amount of numerical integration calculations required by traditional polynomial methods, and the computational efficiency increases significantly.…”
Section: Introductionmentioning
confidence: 99%
“…Vignjevic et al [32] and Destrade [8] attempted to inspect the surface waves as well as shock waves in orthotropic elastic materials. The propagation of surface waves in orthotropic composite structure with irregular interfaces has been studied by Singh and Alam [29] whereas Othmani et al [20] investigated the guided waves propagation in orthotropic viscoelastic carbon-epoxy plate by Legendre polynomial method. Some significant works were studied by Kaushik and Chopra [15] as well as Gogna and Chander [14] based on reflection and transmission of general plane SH-waves at the plane interface between two heterogeneous homogeneous viscoelastic media and anisotropic inhomogeneous viscoelastic half-spaces respectively.…”
Section: Introductionmentioning
confidence: 99%