Null Field Torsion.1

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  • 7/28/2019 Null Field Torsion.1

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    Copyright c 2006 Tech Science Press CMES, vol.12, no.2, pp.109-119, 2006

    Analysis of Circular Torsion Bar with Circular Holes Using Null-eld Approach

    Jeng-Tzong Chen 1 , Wen-Cheng Shen 2, Po-Yuan Chen 2

    Abstract: In this paper, we derive the null-eld inte-gral equation for a circular bar weakened by circular cav-ities with arbitrary radii and positions under torque. Tofully capture the circular geometries, separate forms of fundamental solution in the polar coordinate and Fourierseries for boundary densities are adopted. The solutionis formulated in a manner of a semi-analytical form sinceerror purely attributes to the truncation of Fourier series.Torsion problems are revisited to demonstrate the validityof our method. Torsional rigidities for different numberof holes are also discussed.

    keyword: Torsion, Null-eld integral equation,Fourier series, Circular hole, Torsional rigidity.

    1 Introduction

    Boundary value problems always involve several holesor more than one important reference point. It is con-venient to be able to expand the solutions in alternative

    ways, each way referring to different specic coordinateset describing the same solution. According to the idea,we develop a systematic approach including the adaptiveobserver system and degenerate kernel for fundamentalsolution in the polar coordinate and employ Fourier se-ries to approximate the boundary data.

    In the past, multiply connected problems have been car-ried out either by conformal mapping or by special tech-niques. Ling [Ling C. B. (1947)] solved the torsionproblem of a circular tube with several holes. Muskhel-ishvili [Muskhelishvili N. I. (1953)] solved the problem

    of a circular bar reinforced by an eccentric circular in-clusion. Chen and Weng [Chen T.; Weng I. S. (2001)]have introduced conformal mapping with a Laurent se-ries expansion to analyze the Saint-Venant torsion prob-lem. They concerned with a eccentric bar of different ma-

    1 Distinguished Professor, Department of Harbor and River En-gineering, National Taiwan Ocean University, Keeling, Taiwan.Email: [email protected]

    2 Graduate student, Department of Harbor and River Engineering,National Taiwan Ocean University, Keeling, Taiwan.

    terials with an imperfect interface under torque. Basedon the CVBEM (complex variable boundary elementmethod), Shams-Ahmadi and Chou [Shams-Ahmadi M.;Chou S. I. (1997)] have investigated the torsion prob-lem of composite shafts with any number of inclusionsof different materials. Recently, Ang and Kang [AngW. T.; Kang I. (2000)] developed a general formulationfor solving the second-order elliptic partial differentialequation for a multiply-connected region in a differentversion of CVBEM. To avoid mesh generation for niteelement or boundary element, meshless formulation isa promising direction [Jin B. (2004), Sladek V.; Sladek J.; Tanaka M. (2005), Wordelman C. J.; Aluru N. R.;Ravaioli U. (2000)]. The present formulation can beseen as one kind of meshless methods, since it belongsto boundary collocation methods. Because the confor-mal mapping is limited to the doubly connected region,an increasing number of researchers have paid more at-tentions on special solutions. However, the extensionto multiple circular holes may encounter difculty. It

    is not trivial to develop a systematic method for solv-ing the torsion problems with several holes. Crouch andMogilevskaya [Crouch S. L.; MogilevskayaS. G. (2003)]utilized Somiglianas formula and Fourier series for elas-ticity problems with circular boundaries. Mogilevskayaand Crouch [Mogilevskaya S. G.; Crouch S. L. (2001)]have solved the problem of an innite plane containingarbitrary number of circular inclusionsbased on the com-plex singular integral equation. In their analysis pro-cedure, the unknown tractions are approximated by us-ing the complex Fourier series. However, for calculat-

    ing an integral over a circular boundary, they didnt ex-press the fundamental solution using the local polar co-ordinate. By moving the null-eld point to the bound-ary, the boundary integral can be easily determined us-ing series sums in our formulation due to the introduc-tion of degenerate kernels. Mogilevskaya and Crouch[Mogilevskaya S. G.; Crouch S. L. (2001)] have used theGalerkin method to approach boundary density insteadof collocation approach. Our approach can be extendedto the Galerkin formulation only for the circular and an-