Predicting dynamic response of stiffened-plate composite structures in a wide-frequency domain based on Composite B-spline Wavelet Elements Method (CBWEM)

https://doi.org/10.1016/j.ijmecsci.2018.06.031Get rights and content

Highlights

  • The new numerical scheme is derived for coupling the c1 type substructures.

  • CBWEM is proposed for modeling stiffened-plate composite structures.

  • CPU time to predict the dynamic response in wide frequency domain is 3.5 s.

  • The CBWEM can be taken as a new technique to solve mid-frequency problem.

Abstract

Due to the mid-frequency problem, the Hybrid Statistical Energy Analysis (SEA) / Traditional Finite Element Methods (TFEMs) methods still cannot provide the dynamic responses of the stiffened-plate composite structures in a wide frequency domain. The main reason is that all of the SEA and TFEMs cannot provide the reliable numerical solutions in the middle frequency domain when simulating the thin plate substructures. In order to solve the problem, this paper proposes the Composite B-spline Wavelet Elements Method (CBWEM) based on the c1 type wavelet plate and beam elements for modeling the stiffened-plate composite structures and predicting its dynamic responses in a wide frequency domain. Unfortunately, due to the complex interpolation functions and transformation matrices of these c1 type wavelet elements, the existing numerical scheme to construct the constraint matrix will be invalid when modeling the coupling relationship between the c1 type wavelet plate and beam elements. To solve the problem, this study deduces and gives the formulas of the new numerical scheme for constructing the constraint matrix and modeling the stiffened-plate composite structures based on the CBWEM. Besides, the numerical and experimental studies are carried out to verify the CBWEM, respectively. On the one hand, the numerical study displays that the proposed method can solve the mid-frequency problem and provide reliable dynamic responses in a wide frequency domain within an acceptable computational cost. On the other hand, the experimental study shows that the Central Processing Unit (CPU) time to predict the dynamic response in a wide frequency domain is less than 3.5 s only based on the proposed method and the personal computers, and the corresponding numerical solutions are in good agreement with the experimental results. Thus, we can easily conclude that the proposed method can be taken as one useful numerical technique to solve the mid-frequency problem and predict the dynamic responses of the stiffened-plate composite structures in a wide frequency domain.

Introduction

The stiffened-plate composite structures have been widely applied in various products, such as aerofoil, submarine, rocket, carriage, ships and etc, in engineering [1]. And, people have paid more and more attention on these products’ better sound and vibration performance. According to the theory of the dynamic analysis, to capture better sound and vibration performance, it is necessary to predict the stiffened-plate composite structures’ dynamic response in a wide frequency domain, nowadays. However, due to the mid-frequency problem [2], the existing methods, such as Traditional Finite Element Methods (TFEMs), Statistical Energy Analysis (SEA) and the Hybrid SEA/TFEMs methods, still cannot be applied for providing the reliable numerical solutions of the dynamic responses in a wide frequency domain [3], [4], [5]. Furthermore, according to the Mace et al. [6], the mid-frequency problem is one significant obstacle when improving the stiffened-plate composite structures’ sound and vibration performance. Thus, it is necessary to solve the mid-frequency problem and predict the dynamic response in a wide frequency domain when simulating the stiffened-plate composite structures for improving its sound and vibration performance.

Nowadays, in order to solve the mid-frequency problem and predict the dynamic responses of the stiffened-plate composite structures in a wide frequency domain, many researchers have paid their attention on proposing the efficient numerical methods for providing the reliable dynamic solutions in the mid-frequency domain. According to the Yin and coworkers [3], [4], [7], [8], [9], [10], [11], [12], [13], [14], [15], [16], [17], we can easily find that the Hybrid TFEMs/SEA methods have been widely applied for solving the mid-frequency problem and providing the dynamic solutions of the stiffened-plate composite structures, nowadays. Moreover, these Hybrid SEA/TFEMs methods have become the most popular numerical methods in the field of sound and vibration analysis when predicting the stiffened-plate composite structures’ dynamic responses in a wide frequency domain. And, these Hybrid TFEMs/SEA methods hold great attraction in the field of sound and vibration analysis. However, it is should be noted that there still exist some noticeable problems in the process of dynamic analysis by these Hybrid SEA\TFEMs methods.

Firstly, in order to proceed dynamic analysis based on these Hybrid SEA/TFEMs methods in a wide frequency domain, the stiffened-plate composite structures must be divided into the SEA substructures and the TFEMs substructures, respectively. Secondly, the coupling algorithm to connect the SEA and TFEMs substructures must be given for simulating the coupling effect between the stiffener and thin plate substructures. Thirdly, in order to apply these Hybrid SEA/TFEMs methods for proceeding dynamic analysis, the engineers must master the TFEMs and SEA technologies, simultaneously. Besides, there does still exist a difficult question when applying these Hybrid SEA/TFEMs methods for proceeding dynamic response in a wide frequency domain. That is the mid-frequency problem. Thus, these Hybrid TFEMs/SEA methods still cannot provide the reliable numerical solutions in a wide frequency domain in practice, efficiently [3].

It is mainly due to that these Hybrid TFEMs/SEA methods are validity only when the stiffener and thin plate substructures of the stiffened-plate composite structures can be simulated efficiently based on TFEMs and SEA, respectively. Although the stiffener always can be simulated efficiently based on the TFEMs in the bandwidth, due to the limitation of the SEA, the thin plate substructures still cannot be simulated efficiently in the low and middle frequency domain. Thus, we can clearly conclude that due to the mid-frequency problem, these Hybrid SEA/TFEMs methods always cannot provide reliable numerical solutions in a wide frequency domain when modeling the stiffened-plate composite structures [18]. Besides, these Hybrid SEA/TFEMs methods only can give the trends of the dynamic responses in the analyzing bandwidth without the detailed information, such as the resonance peak. It is one significant obstacle to improve the products’ sound and vibration performance. Therefore, we can easily conclude that it is still necessary to break up the limitation of SEA or TFEMs and solve the mid-frequency problem when predicting the stiffened-plate composite structures’ dynamic responses in a wide frequency domain only based on SEA or TFEMs.

Comprehensive the above contents and the relevant Refs. [2], [6], on the one hand, because of the theoretical restrictions, the SEA only can provide the reliable dynamic responses in the high-frequency domain and cannot provide the reliable numerical solutions in the low to middle frequency domain. On the other hand, because of the low computing accuracy and huge computational cost, the TFEMs only can provide the reliable dynamic solutions in the low-frequency domain and cannot provide the reliable numerical solutions in the middle to high frequency domain. By analyzing these two kinds of reasons why the mid-frequency problem still exists in practice, we can clearly conclude that there is a theoretical limit to solve the mid-frequency problem based on SEA. Therefore, by analyzing these two kinds of numerical methods, we consider that the methods based on the theory of finite element still provide the potential to solve the mid-frequency problem and provide the reliable dynamic solutions in a wide frequency domain. Based on this, we can easily conclude that once the low computational accuracy and huge computational cost of the TFEMs can be overcome efficiently, the methods based on the theory of the finite element method can be applied for solving the mid-frequency problem and providing the reliable dynamic solutions in a wide-frequency domain when simulating the stiffened-plate composite structures. Based on this view, this paper will focus on proposing the Composite B-spline Wavelet Elements Method (CBWEM) derived from the Wavelet Element Methods (WFEMs) which own much better computational efficiency and accuracy compared with the TFEMs. Therefore, the B-spline wavelet and the theory of finite element method will be introduced into this paper for capturing the excellent computing efficiency and accuracy.

On the one hand, for the B-spline and wavelet functions, by observing the relevant researches, we can easily find that these functions own the excellent properties of multi-resolution and the multi-scale when proceeding the numerical analysis or signal processing [19], [20]. And until to now, the B-spline and wavelet functions have been introduced into various applications. Among these, the adaptive wavelet methods were developed for solving the hardening problem in elastoplasticity [21]. And, the non-uniform rational B-splines were applied for producing the basis functions and constructing an exact geometric model [22]. Later, a Reissner–Mindlin shell formulation based on a degenerated solid is implemented for non-uniform rational B-splines based isogeometric analysis [23]. And, in the field of mathematics, the cubic B-spline wavelets were introduced to reduce the fractional Integro-differential equation to system of algebraic equations [24]. By observing these researches, it is obvious that the B-spline and wavelet functions own much better advantages for proceeding the numerical analysis. On the other hand, based on the Chen and coworkers [25], [26], [27], [28], [29], [30], [31], [32], [33], [34], we can clearly find that the WFEMs based on the B-spline and the finite element method own excellent computational efficiency (low computational cost and much better computing accuracy) compared with the TFEMs. And, the WFEMs was applied for quantitative crack identification by using particle swarm optimization [35], and the Hybrid method combing the B-spline wavelet finite element method and spectral analysis was proposed to investigate the wave propagation [36]. Recently, the high frequency response of the thin plate structures with uncertain parameters also has been simulated successfully and efficiently based on the B-spline wavelet finite element method [37].

Therefore, we can easily conclude that the proposed method based on the WFEMs may provide the potential to solve the mid-frequency problem caused by the low computing accuracy and huge computational cost when predicting the stiffened-plate composite structures’ dynamic responses based on the TFEMs. According to the theory of finite element method, in order to simulate the stiffened-plate composite structures based on the c1 type wavelet elements, this research introduces the c1 type B-spline wavelet beam and thin plate elements and applies these elements for modeling the stiffener and thin plate substructures of the stiffened-plate composite structures, respectively. Evidently, the stiffened-plate composite structures can be simulated by these two c1 types wavelet element only when the suitable constraint matrix CBSWI being constructed efficiently. Unfortunately, due to the complex interpolation functions and transformation matrices of these two c1 types B-spline wavelet elements [38], the constraint matrix CBSWI cannot be constructed based on the existing numerical scheme. In order to solve the problem, this paper derives the formulas of the new numerical scheme for constructing the properly constraint matrix CBSWI and applies the CBWEM for solving the mid-frequency problem and predicting the dynamic responses of the stiffened-plate composite structures in a wide frequency domain.

Evidently, there are two main research contents in this paper: (a) deducing the essential formulas of the new numerical scheme for constructing the properly constraint matrix CBSWI; (b) proposing the CBWEM based on the constraint matrix CBSWI and the c1 type B-spline wavelet plate and beam elements for solving the mid-frequency problem and predicting the dynamic response of the stiffened-plate composite structures in a wide frequency domain. In order to introduce these two main research contents, this study will be organized as follows.

Firstly, in order to make readers more than understand this article mainly contents, the formulas to construct the c1 type B-spline wavelet plate and beam elements will be introduced briefly. Secondly, the essential formulas of the new numerical scheme to construct the CBSWI and the CBWEM to proceed dynamic analysis will be deduced and introduced carefully. Lastly, the numerical and experimental studies are adopted for verifying the CBWEM's prediction ability to solve the mid-frequency problem and predict the dynamic responses of the stiffened-plate composite structures in a wide frequency domain.

Section snippets

The c1 type B-spline wavelet elements

In this section, on the one hand, the formulas to construct the c1 type B-spline wavelet beam and plate elements will be introduced briefly. On the other hand, the reasons why the existing numerical scheme to construct the constraint matrix CBSWI are invalid will be introduced carefully.

In order to construct the c1 type B-spline wavelet beam element, as shown in Fig. 1, one-dimensional wavelet scaling function will be taken as the interpolation function instead of one-dimensional traditional

The formulas of the CBWEM

In this section, the formulas of the new numerical scheme to construct the constraint matrix CBSWI and perform the CBWEM will be derived and introduced carefully. As mention above, once the constraint matrix CBSWI can be given completely the global stiffness matrix Kstiffened-plate and mass matrix Mstiffened-plate of the finite element model of the stiffened-plate composite structures can be given by Kstiffenedplate=Kp+CBSWITKbCBSWIMstiffenedplate=Mp+CBSWITMbCBSWI

And then, the CBWEM to solve

Numerical studies

In this section, the stiffened-plate composite structures will be taken as the numerical examples to verify the proposed method. For the aim of the paper and the research purpose, the numerical studies will include three aspects: (a) verifying the CBWEM's prediction ability to solve the mid-frequency problem; (b) verifying the CBWEM's prediction ability to predict the dynamic response in a wide frequency domain; (c) convergence study to investigate the proposed method's numerical stability.

Experimental studies

As mentioned earlier, the Hybrid SEA/TFEMs methods are the most popular numerical methods to predict the dynamic response of stiffened-plate composite structures in a wide frequency domain, especially in the high-frequency domain, nowadays. Thus, in order to illustrate the proposed method's validity and its advantages, the comparative analysis based on the Hybrid SEA/TFEMs method and the CBWEM will be adopted in the experimental studies. In this section, the 1/3rd octave will be adopted for

Conclusion

In order to solve the mid-frequency problem and predict the stiffened-plate composite structures’ dynamic response in a wide frequency domain, this paper derived the essential formulas of the new numerical scheme to construct the constraint matrix CBSWI for coupling the c1 type B-spline wavelet plate and beam elements and proposed the CBWEM for proceeding the dynamic analysis of the stiffened-plate structures. Later, the prediction ability of the CBWEM is investigated by the numerical and

Acknowledgments

This work was supported by the National Natural Science Foundation of China (Nos. 51775408 & 51405370), the National Key Basic Research Program of China (No. 2015CB057400) and the Project Funded by Key Laboratory of Product Quality Assurance & Diagnosis (No. 2014SZS14-P05).

References (45)

  • H. Yin et al.

    Hybrid finite element/statistical energy method for mid-frequency analysis of structure−acoustic systems with interval parameters

    J Sound Vib

    (2015)
  • F. Wu et al.

    A novel hybrid ES-FE-SEA for mid-frequency prediction of transmission losses in complex acoustic systems

    Appl Acoust

    (2016)
  • Y. Fan et al.

    Energy flow prediction in built-up structures through a hybrid finite element/wave and finite element approach

    Mech Syst Signal Proecss

    (2016)
  • A. Seçgin et al.

    A modal impedance technique for mid and high frequency analysis of an uncertain stiffened composite plate

    J Sound Vib

    (2016)
  • J. Xiang et al.

    The construction of plane elastomechanics and Mindlin plate elements of B-spline wavelet on the interval

    Finite Elem Anal Des

    (2006)
  • T.J.R. Hughes et al.

    Isogeometric analysis: CAD, finite elements, NURBS, exact geometry and mesh refinement

    Computer Methods Appl Mech Eng

    (2005)
  • D.J. Benson et al.

    Isogeometric shell analysis: The Reissner Mindlin shell

    Comput Methods Appl Mech Engrg

    (2010)
  • X. Chen et al.

    The construction of wavelet finite element and its application

    Finite Elem Anal Des

    (2004)
  • X. Zhang et al.

    The analysis of shallow shells based on multivariable wavelet finite element method

    Acta Mech Solida Sin

    (2011)
  • Z. Yang et al.

    Free vibration and buckling analysis of plates using B-spline wavelet on the interval Mindlin element

    Appl Math Model

    (2013)
  • H. Zuo et al.

    Analysis of laminated composite plates using wavelet finite element method and higher-order plate theory

    Compos Struct

    (2015)
  • X. Zhang et al.

    Analysis of shallow hyperbolic shell by different kinds of wavelet elements based on B-spline wavelet on the interval

    Appl Math Model

    (2016)
  • Cited by (12)

    • A wavelet method for large-deflection bending of irregular plates

      2023, International Journal of Mechanical Sciences
    • A homotopy-based wavelet method for extreme large bending analysis of heterogeneous anisotropic plate with variable thickness on orthotropic foundation

      2023, Applied Mathematics and Computation
      Citation Excerpt :

      Wavelets [27,28] have been recently developed and extensively used in analyzing different mechanical properties of plate involving elastic bending [29,30], buckling [31], vibration [32] and impact [33], owing to its advantage in local characterization of deformation and motion by reasonable selection of appropriate primary function. Various researchers have exploited the potential of wavelet basis functions and proposed many wavelet-based solution methods for plate mechanical issues [34], such as wavelet Galerkin method [35–37], wavelet collocation method [29], wavelet boundary element method [38], wavelet finite element method [39,40], wavelet spectral finite element [41], closed wavelet method [42], integration modified wavelet neural networks [43], trigonometric wavelet-based method [44] and finite wavelet domain method [45]. It is remarkable that the wavelet homotopy method [46] inherits the merits of Homotopy Analysis Method (HAM) in dealing strongly nonlinear problems but also possesses high-precision properties in wavelet approximation, which is one of the best alternative approaches applied in solving nonlinear Bratu equation [47], Von Kármán equations [48] and nonlinear bending of plates [49,50].

    • Large deflection bending analysis of variable-thickness tapered plates under three-dimensionally hygrothermomechanical loads

      2021, International Journal of Mechanical Sciences
      Citation Excerpt :

      Due to its powerful mathematical multi-resolution analysis characterizing the detailed properties of functions in hierarchical and nested subspaces, wavelet has been an important tool to deal with mechanical problems [53,54]. Many wavelet-based methods have been proposed to investigate static and dynamic properties of plates, such as wavelet finite element method [55–58], meshless local Petrov-Galerkin method [59], wavelet collocation method [60,61], trigonometric wavelet-based method [62], integration modified wavelet neural networks [63], wavelet spectral finite element method [64], integrated wavelet transform and hybrid minimization algorithm [65], composite B-spline wavelet elements method (CBWEM) [66], closed wavelet method [67], wavelet integral collocation method [68], simultaneous space-time wavelet method [69] and wavelet homotopy method [70–72]. In view of published work [43,49–52], most researches of variable-thickness tapered plate in linearly hygrothermomechanical bending are limited in small deflection with weaker nonlinearity.

    View all citing articles on Scopus
    View full text