1. M M S S V V 0 Scattering of flexural wave in a thin plate with multiple circular inclusions by using the multipole Trefftz method Wei-Ming Lee 1, Jeng-Tzong Chen 2, Hung-Ho Hsu 1 1 Department of Mechanical Engineering, China University of Science and Technology, Taipei, Taiwan 2 Department of Harbor and River Engineering, National Taiwan Ocean University, Keelung, Taiwan 2009 年 11 月 14 日國立聯合大學

2. M M S S V V 1 Outlines 4. Concluding remarks 3. Illustrated examples 2. Methods of solution 1. Introduction

3. M M S S V V 2 Outlines 4. Concluding remarks 3. Illustrated examples 2. Methods of solution 1. Introduction

4. M M S S V V 3 Introduction Inclusions, or inhomogeneous materials, usually take place in shapes of discontinuity such as thickness reduction or strength degradation. The deformation and corresponding stresses caused by the dynamic force are induced throughout the structure by means of wave propagation.

5. M M S S V V 4 Scattering At the irregular interface of different media, stress wave reflects in all directions scattering The near field scattering flexural wave results in the dynamic stress concentration which will reduce loading capacity and induce fatigue failure. Certain applications of the far field scattering flexural response can be obtained in vibration analysis or structural health-monitoring system.

6. M M S S V V 5 Literature review From literature reviews, few papers have been published to date reporting the scattering of flexural wave in plate with more than one inclusion. In 1932, Trefftz presented the Trefftz method categorized as the boundary-type solution such as the BEM or BIEM which can reduce the dimension of the original problem by one. The Trefftz formulation is regular and free of calculating improper boundary integrals.

7. M M S S V V 6 Objective The concept of multipole method to solve multiply scattering problems was firstly devised by Zavika in 1913. Our objective is to develop an analytical approach to solve the scattering problem of flexural waves in an infinite thin plate with multiple circular inclusions by combining the Trefftz method and the multipole method.

8. M M S S V V 7 Outlines 4. Concluding remarks 3. Illustrated examples 2. Methods of solution 1. Introduction

9. M M S S V V 8 For time-harmonic motion, the governing equation of motion for the plate is the out-of-plane displacement is the wave number is the biharmonic operator is the unbounded exterior plate w(x)w(x) ω is the angular frequency D is the flexural rigidity h is the plates thickness E is the Young’s modulus μ is the Poisson’s ratio ρ is the surface density

10. M M S S V V 9 Problem Statement Problem statement for an infinite plate containing multiple circular inclusions subject to an incident flexural wave

11. M M S S V V 10 The integral representation for the plate problem

12. M M S S V V 11

13. M M S S V V 12 The slope, moment and effective shear operators slope Normal moment effective shear Tangential moment

14. M M S S V V 13 Analytical derivations for flexural wave scattered by multiple circular inclusions The scattered field of plate can be expressed as an infinite sum of multipole The displacement field of the plate is

15. M M S S V V 14 The displacement field of the pth inclusion is expressed as

16. M M S S V V 15 The continuity conditions

17. M M S S V V 16 For the pth circular displacement continuity (1) The higher order derivatives (2) Several different variables

18. M M S S V V 17 x Addition Theorem

19. M M S S V V 18

20. M M S S V V 19 The interface displacement continuity

21. M M S S V V 20 The interface slope continuity

22. M M S S V V 21 The interface bending moment continuity

23. M M S S V V 22 The interface shear force continuity

24. M M S S V V 23 The analytical model for the flexural scattering of an infinite plate containing multiple circular inclusions

25. M M S S V V 24 Outlines 4. Concluding remarks 3. Illustrated examples 2. Methods of solution 1. Introduction

26. M M S S V V 25 Case 1: An infinite plate with one inclusion Geometric data: R 1 =1m Thickness Plate:0.002m Distribution of DMCF on the circular boundary (ka=0.005, h/h 0 =0.0005) 1.8514

27. M M S S V V 26 Distribution of DMCF on the circular boundary ka=0.5 ka=1.0 ka=3.0

28. M M S S V V 27 Far-field backscattering amplitude

29. M M S S V V 28 Case 2: An infinite plate with two inclusions

30. M M S S V V 29 Distribution of DMCF on the circular boundary (L/a=2.1) ka=0.5 ka=1.0 ka=3.0

31. M M S S V V 30 Far-field backscattering amplitude (L/a=2.1)

32. M M S S V V 31 Distribution of DMCF on the circular boundary (L/a=4.0) ka=0.5 ka=1.0 ka=3.0

33. M M S S V V 32 Far-field backscattering amplitude (L/a=4.0)

34. M M S S V V 33 Outlines 4. Concluding remarks 3. Illustrated examples 2. Methods of solution 1. Introduction

35. M M S S V V 34 Concluding remarks An analytical approach to solve the scattering problem of flexural waves and to determine the DMCF and the far field scattering amplitude in an infinite thin plate with multiple circular inclusions was proposed By using the addition theorem, the Trefftz method can be extended to deal with multiply scattering problems. The magnitude of DMCF of two inclusions is larger than that of one when the space of inclusions is small. The proposed algorithm is general and easily applicable to problems with multiple inclusions which are not easily solved by using the traditional analytical method. 1. 2. 3. 4. 5. The effect of the space between inclusions on the near-field DMCF is different from that on the far-field scattering amplitude.

36. M M S S V V 35 Thanks for your kind attention The End