請用此 Handle URI 來引用此文件:
http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/73145完整後設資料紀錄
| DC 欄位 | 值 | 語言 |
|---|---|---|
| dc.contributor.advisor | 鍾立來,劉進賢 | |
| dc.contributor.author | Wun-Sin Jhao | en |
| dc.contributor.author | 趙汶欣 | zh_TW |
| dc.date.accessioned | 2021-06-17T07:19:32Z | - |
| dc.date.available | 2022-07-15 | |
| dc.date.copyright | 2019-07-15 | |
| dc.date.issued | 2019 | |
| dc.date.submitted | 2019-07-09 | |
| dc.identifier.citation | [1] Abu-Hilal, M., Forced vibration of Euler-Bernoulli beams by means of dynamic Green functions. Journal of Sound and Vibration. 267(2): p. 191-207, 2003.
[2] Ahn, S., Choi, U.J.,Ramm, A.G., A scheme for stable numerical differentiation. Journal of Computational and Applied Mathematics. 186(2): p. 325-334, 2006. [3] Chopra, Anil, K., Dynamics of structures: theory and applications to earthquake engineering. Prentice-Hall, Englewood Cliffs ,1995. [4] Alemdar Hasanov, O.B., Identification of an unknown spatial load distribution in a vibrating cantilevered beam from final verdetermination. Journal of Inverse and Ill- Posed Problems. 23(1): p. 85-102, 2014. [5] Alves, C., Silvestre, A.L., Takahashi, T.,Tucsnak, M., Solving inverse source problems using observability. applications to the Euler-Bernoulli plate equation. Siam Journal on Control and Optimization. 48(3): p. 1632-1659, 2009. [6] Al-Khatib, M.J., Grysa, K., Maciag, A., The method of solving polynomials in the beam vibration problems. Journal of Theoretical and Applied Mechanics. 46(2): p. 347-366, 2008. [7] Apuzzo, A., Barretta, R., Luciano, R., de Sciarra, F.M.,Penna, R., Free vibrations of Bernoulli-Euler nano-beams by the stress-driven nonlocal integral model. Composites Part B-Engineering. 123: p. 105-111, 2017. [8] Ashyralyev, A., Piskarev, S., Covachev, V., Ashurov, R.,Yurtsever, H.A., Wellposed and ill-posed boundary value problems for PDE. Abstract and Applied Analysis, 2012. [9] Ashyralyev, A., Piskarev, S., Covachev, V., Ashurov, R., Yurtsever, H.A.,Erdogan, A.S., Well-Posed and ill-posed boundary value problems for PDE 2013. Abstract and Applied Analysis, 2013. [10] Audley, D.R.,Lee, D.A., Ill-Posed and well-posed problems in system identification. Ieee Transactions on Automatic Control. Ac19(6): p. 738-747, 1974. [11] Aziz, S.,Malik, S.A., Identification of an unknown source term for a time fractional fourth-order parabolic equation. Electronic Journal of Differential Equations, 2016. [12] Badanin, A.,Korotyaev, E., Inverse problems and sharp eigenvalue asymptotics for Euler-Bernoulli operators. Inverse Problems. 31(5), 2015. [13] Barretta, R., Diaco, M., Feo, L., Luciano, R., de Sciarra, F.M.,Penna, R., Stressdriven integral elastic theory for torsion of nano-beams. Mechanics Research Communications. 87: p. 35-41, 2018. [14] Barretta, R., Fabbrocino, F., Luciano, R.,de Sciarra, F.M., Closed-form solutions in stress-driven two-phase integral elasticity for bending of functionally graded nano-beams. Physica E-Low-Dimensional Systems & Nanostructures. 97: p. 13-30, 2018. [15] Barretta, R., Faghidian, S.A., Luciano, R., Medaglia, C.M.,Penna, R., Stressdriven two-phase integral elasticity for torsion of nano-beams. Composites Part B-Engineering. 145: p. 62-69, 2018. [16] Barretta, R., Luciano, R., de Sciarra, F.M.,Ruta, G., Stress-driven nonlocal integral model for Timoshenko elastic nano-beams. European Journal of Mechanics a-Solids. 72: p. 275-286, 2018. [17] Bartoli, I., Marzani, A., di Scalea, F.L.,Viola, E., Modeling wave propagation in damped waveguides of arbitrary cross-section. Journal of Sound and Vibration. 295(3-5): p. 685-707, 2006. [18] Basha, P.M.,Shanthi, V., Fitted mesh method for a weakly coupled system of singularly perturbed reaction-convection-diffusion problems with discontinuous source term. Ain Shams Engineering Journal. 9(4): p. 1089-1101, 2018. [19] Bender, C.M., Orszag, S.A., Advanced mathematical methods for scientists and engineers, McGraw-Hill, New York, 1978. [20] Brebbia, C.A., The boundary element method for engineers. Pentech Press, 1978. [21] Caddemi, S.,Calio, I., The influence of the axial force on the vibration of the Euler-Bernoulli beam with an arbitrary number of cracks. Archive of Applied Mechanics. 82(6): p. 827-839, 2012. [22] Cha, P.D.,Rinker, J.M., Enforcing nodes to suppress vibration along a harmonically forced damped Euler-Bernoulli beam. Journal of Vibration and Acoustics-Transactions of the Asme. 134(5), 2012. [23] Chang, J.D.,Guo, B.Z., Identification of variable spacial coefficients for a beam equation from boundary measurements. Automatica. 43(4): p. 732-737, 2007. [24] Chechile, R.A., Well-posed, ill-posed, and intermediate problems with applications. Journal of Mathematical Psychology. 50(6): p. 583-583, 2006. [25] Chen, Y.M., Lv, Z.R., Cruise1968, J.K., Error estimation of Fourier series expansion and implication to solution accuracy for nonlinear dynamical systems. Journal of Computational and Nonlinear Dynamics. 12(1), 2017. [26] Cruise, T.A., Rizzo, F.J., A direct formulation and numerical solution of the general transient elasto-dynamic Problem. Journal of Mathematical Analysis and Applications 22(1): p. 244-259, 1968. [27] Cui, M.,Geng, F., A computational method for solving third-order singularly perturbed boundary-value problems. Applied Mathematics and Computation. 198(2): p. 896-903, 2008. [28] De Jager, E.M., Jiang, F.R., The theory of singular perturbation, Noth-Holland, Amsterdam, 1996. [29] de Oliveira, J.P.S., Calenzani, A.F.G., Fakury, R.H.,Ferreira, W.G., Elastic critical moment of continuous composite beams with a sinusoidal-web steel profile for lateral-torsional buckling. Engineering Structures. 113: p. 121-132, 2016. [30] Dettman, J.W., Related well-posed and ill-posed problems in partial differential equations. Studies in Applied Mathematics(5): p. 45, 1969. [31] Dong, L., Alotaibi, A., Mohiuddine, S.A.,Atluri, S.N., Computational methods in engineering: A variety of primal & mixed methods, with global & local interpolations, for well-posed or ill-posed BCs. Cmes-Computer Modeling in Engineering & Sciences. 99(1): p. 1-85, 2014. [32] El-Zahar, E.R.,El-Kabeir, S.M.M., A new method for solving singularly perturbed boundary value problems. Applied Mathematics & Information Sciences. 7(3): p. 927-938, 2013. [33] El-Zahar, E.R., Approximate analytical solutions of singularly perturbed fourth order boundary value problems using differential transform method, Journal of King Saud University Science 25(3): p. 257-265, 2013. [34] Ghannadiasl, A.,Ajirlou, S.K., Forced vibration of multi-span cracked Euler-Bernoulli beams using dynamic Green function formulation. Applied Acoustics.148: p. 484-494, 2019. [35] Gladwell, G.M.L., The inverse problem for the Euler-Bernoulli beam. Proceedings of the Royal Society of London Series a-Mathematical Physical and Engineering Sciences. 407(1832): p. 199-218, 1986. [36] Graff, K.F., Wave Motion in Elastic Solids. 1975. [37] Guo, B.Z., On the boundary control of a hybrid system with variable coefficients. Journal of Optimization Theory and Applications. 114(2): p. 373-395, 2002. [38] Guo, H.L., Huang, C.,Zhang, Z.M., Superconvergence of conforming finite element for fourth-order singularly perturbed problems of reaction diffusion type in 1-D. Numerical Methods for Partial Differential Equations. 30(2): p. 550-566, 2014. [39] Han, S.M., Benaroya, H.,Wei, T., Dynamics of transversely vibrating beams using four engineering theories. Journal of Sound and Vibration. 225(5): p. 935-988, 1999. [40] Hanke, M.,Scherzer, O., Inverse problems light: numerical differentiation. American Mathematical Monthly. 108(6): p. 512-521, 2001. [41] Hasanov, A., Identification of an unknown source term in a vibrating cantilevered beam from final overdetermination. Inverse Problems. 25(11), 2009. [42] Hasanov, A.,Baysal, O., Identification of an unknown spatial load distribution in a vibrating cantilevered beam from final overdetermination. Journal of Inverse and Ill-Posed Problems. 23(1): p. 85-102, 2015. [43] Hasanov, A.,Baysal, O., Identification of unknown temporal and spatial load distributions in a vibrating Euler-Bernoulli beam from Dirichlet boundary measured data. Automatica. 71: p. 106-117, 2016. [44] Hasanov, A.,Kawano, A., Identification of unknown spatial load distributions in a vibrating Euler-Bernoulli beam from limited measured data. Inverse Problems. 32(5), 2016. [45] Hasanov, A.,Pektas, B., Identification of an unknown time-dependent heat source term from overspecified Dirichlet boundary data by conjugate gradient method. Computers & Mathematics with Applications. 65(1): p. 42-57, 2013. [46] Huang, C.H.,Shih, C.C., An inverse problem in estimating simultaneously the timedependent applied force and moment of an Euler-Bernoulli beam. Cmes-Computer Modeling in Engineering & Sciences. 21(3): p. 239-254, 2007. [47] Jawson, M.A. Integral equation methods in potential theory. Proceeding of the Royal Society. p. 23-32, 1963. [48] Kadalbajoo, M.K.,Gupta, V., A brief survey on numerical methods for solving singularly perturbed problems. Applied Mathematics and Computation. 217(8): p. 3641-3716, 2010. [49] Kadalbajoo, M.K.,Patidar, K.C., A survey of numerical techniques for solving singularly perturbed ordinary differential equations. Applied Mathematics and Computation. 130(2-3): p. 457-510, 2002. [50] Kanca, F., Baglan, I., Inverse problem for Euler-Bernoulli equation with periodic boundary condition. Filomat. 32(16): p. 5691-5705, 2018. [51] Karaoglu, P.,Aydogdu, M., On the forced vibration of carbon nanotubes via a nonlocal Euler-Bernoulli beam model. Proceedings of the Institution of Mechanical Engineers Part C-Journal of Mechanical Engineering Science. 224(C2): p. 497-503, 2010. [52] Kawano, A., Uniqueness in the identification of asynchronous sources and damage in vibrating beams. Inverse Problems. 30(6): p. 065008-16, 2014. [53] Kerimov, N.B.,Maris, E.A., On the uniform convergence of Fourier series expansions for Sturm-Liouville problems with a spectral parameter in the boundary conditions. Results in Mathematics. 73(3): p. 102, 2018. [54] Kevorkian, J., Cole, J.D., Perturbation methods in applied mathematics, Springer- Verlag, New York, 1981. [55] Kevorkian, J., Cole, J.D., Multiple scale and singular perturbation methods, Springer-Verlag, New York, 1996. [56] Krstic, M., Guo, B.Z., Balogh, A.,Smyshlyaev, A., Control of a tip-force destabilized shear beam by observer-based boundary feedback. Siam Journal on Control and Optimization. 47(2): p. 553-574, 2008. [57] Krstic, M., Magnis, L.,Vazquez, R., Nonlinear stabilization of shock-like unstable equilibria in the viscous Burgers PDE. Ieee Transactions on Automatic Control. 53(7): p. 1678-1683, 2008. [58] Kumar, M.,Tiwari, S., An initial-value technique to solve third-order reactiondiffusion singularly perturbed boundary-value problems. Journal of Computer Mathematics. 89(17): p. 2345-2352, 2012. [59] Lesnic, D., Elliott, L.,Ingham, D.B., Analysis of coefficient indentification problems associated to the inverse Euler-Bernoulli beam theory. Ima Journal of Applied Mathematics. 62(2): p. 101-116, 1999. [60] Li, B.T., Liu, C.S.,Zhu, L.L., Vibration analysis of composite beams with sinusoidal periodically varying interfaces. Zeitschrift Fur Naturforschung Section a-a Journal of Physical Sciences. 73(1): p. 57-67, 2018. [61] Li, W.Y., Wang, G.,Du, J.T., Vibration analysis of conical shells by the improved Fourier expansion-based differential quadrature method. Shock and Vibration, 2016. [62] Liu, C.-S., Cone of non-linear dynamical system and group preserving schemes. International Journal of Non-Linear Mechanics. 36(7): p. 1047-1068, 2001. [63] Liu, C.-S., Atluri SN, A novel time integration method for solving a large system of non-linear algebraic equations. Computed Model Engine Science. 31: p. 71-83, 2008. [64] Liu, C.-S., A Lie-group adaptive differential quadrature method to identify an unknown force in an Euler–Bernoulli beam equation. Acta Mechanica. 223(10): p. 2207-2223, 2012. [65] Liu, C.S., The Lie-group shooting method for singularly perturbed two-point boundary value problems. Computer Modeling in Engineering & Sciences. 15(3): p. 179-196, 2006. [66] Liu, C.S., Preserving constraints of differential equations by numerical methods based on integrating factors. Computer Modeling in Engineering & Sciences. 12(2): p. 83-107, 2006. [67] Liu, C.S., The Lie-group shooting method for solving nonlinear singularly perturbed boundary value problems. Communications in Nonlinear Science and Numerical Simulation. 17(4): p. 1506-1521, 2012. [68] Liu, C.S., An equilibrated method of fundamental solutions to choose the best source points for the Laplace equation. Engineering Analysis with Boundary Elements. 36(8): p. 1235-1245, 2012. [69] Liu, C.S., Solving third-order singularly perturbed problems: exponentially and polynomially fitted trial functions. Journal of Mathematics Research. 8(2): p. 16-24, 2016. [70] Liu, C.-S., A BIEM using the Trefftz test-functions for solving the inverse Cauchy and source recovery problems. Engineering Analysis with Boundary Elements, 62: p. 177-185, 2016. [71] Liu, C.S., A global boundary integral equation method for recovering space-time dependent heat source. Journal of Heat and Mass Transfer. 92: p. 1034-1040, 2016. [72] Liu, C.S., A global domain/boundary integral equation method for the inverse wave source and backward wave problems. Inverse Problems in Science and Engineering 25: p. 506-531, 2016. [73] Liu, C.S., Solving singularly perturbed problems by a weak-form integral equation with exponential trial functions. Applied Mathematics and Computation. 329: p. 154-174, 2018. [74] Liu, C.S.,Atluri, S.N., A fictitious time integration method for the numerical solution of the Fredholm integral equation and for numerical differentiation of noisy data, and its relation to the filter theory. Cmes-Computer Modeling in Engineering & Sciences. 41(3): p. 243-261, 2009. [75] Liu, C.S.,Atluri, S.N., A GL(n, R) differential algebraic equation method for numerical differentiation of noisy signal. Cmes-Computer Modeling in Engineering & Sciences. 92(2): p. 213-239, 2013. [76] Liu, C.S.,Chang, C.W., A real-time Lie-group differential algebraic equations method to solve the inverse nonlinear vibration problems. Inverse Problems in Science and Engineering. 24(9): p. 1569-1586, 2016. [77] Liu, C.S.,Chang, C.W., Solving nonlinear singularly perturbed problems by fractional order exponential trial functions. Applied Mathematics Letters. 83: p. 219-226, 2018. [78] Liu, C.S., Chang, J.R.,Chen, Y.W., The recovery of external force in nonlinear system by using a weak-form integral method. Nonlinear Dynamics. 86(2): p. 987-998, 2016. [79] Liu, C.S.,Li, B.T., An upper bound theory to approximate the natural frequencies and parameters identification of composite beams. Composite Structures. 171: p. 131-144, 2017. [80] Liu, C.S.,Li, B.T., Reconstructing a second-order Sturm-Liouville operator by an energetic boundary function iterative method. Applied Mathematics Letters. 73: p.49-55, 2017. [81] Liu, C.S., Liu, D.J.,Jhao, W.S., Solving a singular beam equation by using a weakform integral equation method. Applied Mathematics Letters. 64: p. 51-58, 2017. [82] Ma, Y.J., Fu, C.L.,Zhang, Y.X., Identification of an unknown source depending on both time and space variables by a variational method. Applied Mathematical Modelling. 36(10): p. 5080-5090, 2012. [83] Mahmoudpour, E., Hosseini-Hashemi, S.H.,Faghidian, S.A., Nonlinear vibration analysis of FG nano-beams resting on elastic foundation in thermal environment using stress-driven nonlocal integral model. Applied Mathematical Modelling. 57: p. 302-315, 2018. [84] Marinov, T.T.,Vatsala, A.S., Inverse problem for coefficient identification in the Euler-Bernoulli equation. Computers & Mathematics with Applications. 56(2): p. 400-410, 2008. [85] Naguleswaran, S., Vibration and stability of an Euler-Bernoulli beam with up to three-step changes in cross-section and in axial force. International Journal of Mechanical Sciences. 45(9): p. 1563-1579, 2003. [86] Naguleswaran, S., Transverse vibration of an uniform Euler-Bernoulli beam under linearly varying axial force. Journal of Sound and Vibration. 275(1-2): p. 47-57, 2004. [87] Naguleswaran, S., Transverse vibration and stability of an Euler-Bernoulli beam with step change in cross-section and in axial force. Journal of Sound and Vibration. 270(4-5): p. 1045-1055, 2004. [88] Nicaise, S.,Zair, O., Determination of point sources in vibrating beams by boundary measurements: identifiability, stability, and reconstruction results. Electronic Journal of Differential Equations. 2004(20): p. 1-17, 2004. [89] O’Malley, R.E., Singular perturbation methods for ordinary differential equations, Springer-Verlag, New York, 1991. [90] Oskouie, M.F., Ansari, R.,Rouhi, H., Bending of Euler-Bernoulli nanobeams based on the strain-driven and stress-driven nonlocal integral models: a numerical approach. Acta Mechanica Sinica. 34(5): p. 871-882, 2018. [91] Papanicolaou, V.G.,Kravvaritis, D., An inverse spectral problem for the Euler-Bernoulli equation for the vibrating beam. Inverse Problems. 13(4): p. 1083-1092, 1997. [92] Petrovic, P.,Damljanovic, N., Dynamic phasors estimation based on Taylor-Fourier expansion and gram matrix representation. Mathematical Problems in Engineering, 2018. [93] Prabha, T., Chandru, M.,Shanthi, V., Hybrid difference scheme for singularly perturbed reaction-convection-diffusion problem with boundary and interior layers. Applied Mathematics and Computation. 314: p. 237-256, 2017. [94] Ramm, A.G.,Smirnova, A.B., On stable numerical differentiation. Mathematics of Computation. 70(235): p. 1131-1153, 2001. [95] Richard, M.C., Mechanics of composite materials. John Wiley and Sons, New York, 1979. [96] Robert, J.M., Mechanics of composite materials. Hemisphere, New York, 1975. [97] Roja, J.C.,Tamilselvan, A., Numerical method for singularly perturbed third order ordinary differential equations of convection-diffusion type. Numerical Mathematics-Theory Methods and Applications. 7(3): p. 265-287, 2014. [98] Romano, G.,Barretta, R., Stress-driven versus strain-driven nonlocal integral model for elastic nano-beams. Composites Part B-Engineering. 114: p. 184-188, 2017. [99] Romano, G.,Barretta, R., Nonlocal elasticity in nanobeams: the stress-driven integral model. International Journal of Engineering Science. 115: p. 14-27, 2017. [100] Roos, H.G., Stynes, M., Tobiska, L., Numerical methods for singularly perturbed differential equations, Springer-Verlag, Berlin, 1996. [101] Nayfeh, A.H., Introduction to perturbation techniques. Wiley, New York, 1981. [102] Sakar, G., The effect of axial force on the free vibration of an Euler-Bernoulli beam carrying a number of various concentrated elements. Shock and Vibration. 20(3): p. 357-367, 2013. [103] Schoeftner, J.,Irschik, H., Passive shape control of force-induced harmonic lateral vibrations for laminated piezoelastic Bernoulli-Euler beams-theory and practical relevance. Smart Structures and Systems. 7(5): p. 417-432, 2011. [104] Shanthi, V.,Ramanujam, N., Asymptotic numerical methods for singularly perturbed fourth order ordinary differential equations of convection-diffusion type. Applied Mathematics and Computation. 133(2-3): p. 559-579, 2002. [105] Shanthi, V.,Ramanujam, N., A numerical method for boundary value problems for singularly perturbed fourth-order ordinary differential equations. Applied Mathematics and Computation. 129(2-3): p. 269-294, 2002. [106] Shanthi, V.,Ramanujam, N., Asymptotic numerical methods for singularly perturbed fourth-order ordinary differential equations of reaction-diffusion type. Computers & Mathematics with Applications. 46(2-3): p. 463-478, 2003. [107] Shanthi, V.,Ramanujam, N., A boundary value technique for boundary value problems for singularly perturbed fourth-order ordinary differential equations. Computers & Mathematics with Applications. 47(10-11): p. 1673-1688, 2004. [108] Shanthi, V.,Ramanujam, N., Asymptotic numerical method for boundary value problems for singularly perturbed fourth-order ordinary differential equations with a weak interior layer. Applied Mathematics and Computation. 172(1): p. 252-266, 2006. [109] Shin, Y.J.,Yun, J.H., Transverse vibration of a uniform Euler-Bernoulli beam under varying axial force using differential transformation method. Journal of Mechanical Science and Technology. 20(2): p. 191-196, 2006. [110] Sih, C.G., Application of Fracture-Mechanics to Composite-Material Failure. Experimental Mechanics. 19(5): p. N40-N40, 1979. [111] Sinir, S., Cevik, M.,Sinir, B.G., Nonlinear free and forced vibration analyses of axially functionally graded Euler-Bernoulli beams with non-uniform cross-section. Composites Part B-Engineering. 148: p. 123-131, 2018. [112] Shampine, L.F., Gear, C.W., A user’s view of solving stiff ordinary differential equations, SIAM Rev. 21: p. 1-17, 1979. [113] Symm, G.T., Integral equation methods in potential theory II. Proceeding of the Royal Society A 25. p. 33-46, 1963. [114] Valarmathi, S.,Ramanujam, N., A computational method for solving boundary value problems for third-order singularly perturbed ordinary differential equations. Applied Mathematics and Computation. 129(2-3): p. 345-373, 2002. [115] Walczak, S., Well-posed and ill-posed optimal control problems. Journal of Optimization Theory and Applications. 109(1): p. 169-185, 2001. [116] Wang, X.H.,Shirinzadeh, B., High-order nonlinear differentiator and application to aircraft control. Mechanical Systems and Signal Processing. 46(2): p. 227-252, 2014. [117] Zhang, Z.H., Fourier expansions with polynomial terms for random processes. Journal of Function Spaces, 2015. [118] Zhao, X., Zhao, Y.R., Gao, X.Z., Li, X.Y.,Li, Y.H., Green’s functions for the forced vibrations of cracked Euler-Bernoulli beams. Mechanical Systems and Signal Processing. 68-69: p. 155-175, 2016. | |
| dc.identifier.uri | http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/73145 | - |
| dc.description.abstract | 本論文發展出五套數值方法分別求解尤拉梁偏微分方程式的正反算問題,此正反算問題係屬於病態問題,乃是因為其解若存在,而其解卻不連續仰賴於量測數據點,而若因量測數據具有微量的干擾,其解必產生極大的誤差。雖有學者提出許多的改善此病態問題之方法,病態問題卻未能有效改善。於正算問題中,本文發展出兩套方法,分別為弱形式積分方程法以及配點法求解奇異攝動梁問題;在反算問題上,本文發展出三套方法,分別為穩定數值噪音數據微分器、非迭代之空間恢復力法以及邊界泛函法求解外力源恢復之梁問題。
奇異攝動梁問題指其材料本身之剛性遠小於外部張力之作用,因而衍伸出小參數的問題,但此問題不能夠直接以把小參數設為零而求近似解。若依常規攝動法把小參數設為零,將會導致方程降階,而不得該問題的近似解,故此為微小參數之變動所造成的病態問題。弱形式積分方程法先對四階常微分方程式採用弱形式方法進行積分,建構一個測試函數滿足梁的邊界,將常微分方程式的微分運算子利用分部積分法,將運算子作用於連續且可微之伴隨邊界測試函數上,並進一步推導出線性系統求解試函數的未知係數,此係數帶回即得梁位移之函數。指數多項式函數之配點法不同於弱形式積分方程法,此法採用指數多項式函數為解之基底,針對佈點代回四階常微分方程式而導出線性系統求解試函數的未知係數,此係數代回即得梁位移之函數。 梁外力恢復問題係指在已知位移而外力源未知之反算問題。此反算問題若於量測位移數據具有微量的干擾,再對其噪音數據微分,其外力源恢復的結果必產生極大的誤差。本文基於反算病態問題,提出穩定數值噪音數據微分器,此法運用了弱形式積分方程法之概念來解決數據微分噪音的反算問題,建構一個滿足邊界方程式的測試函數,並導入邊界型函數之概念,使外力試函數更具有彈性去描述外力源問題。非迭代之空間恢復力法,先採格林第二恆等式將域問題轉為邊界積分問題,透過選取伴隨特徵函數作為測試函數,在滿足控制方程式以及邊界條件下,此函數還避免了格林函數之奇異性;再者,在巧妙的選擇伴隨特徵函數與外力試函數,此法可求得係數的閉合解析解,在位移數據具有噪音干擾的情況下,有效恢復未知空間外力源問題。邊界泛函法則考量力與位移的功能轉換,並借助量測空間邊界外力作為附加條件,本法導出一系列的空間邊界函數,此空間邊界函數透過與隱格式時間函數的作用下,不僅滿足梁方程式的邊界條件,更能於時間上保守能。在所有邊界函數皆保守能的情況下,可建立一個包含零元素構成的線性空間。透過對線性系統求解空間邊界函數的未知係數,此係數帶回即得梁外力源之函數。 本文透過將空間上與時間上的數據點加入噪音,透過噪音的放大過程,可瞭解數據噪音對於正反算問題的敏感程度,並討論數據噪音在各種梁形式下,試函數以及測試函數展開項次的影響性,進而在描述梁受外力模擬時需仔細考量之因素。最後以解析解與方法論之數值模擬結果比較,驗證本方法論於正反算病態梁問題中,確實可有效且準確地求解空間與時間項的外力恢復源問題與提高計算精度,而對於帶有噪訊干擾的量測數據,進行深入的解析與探討該方法論對解的穩定性與計算誤差。 | zh_TW |
| dc.description.abstract | In this dissertation we investigate the ill-posed problems about the direct problem and the inverse problem in Euler-Bernoulli beam. The solution of direct problem is existent and unique; however, it does not rely on the continuously measurement data. On the other hand, the inverse problem, deducing a force distribution from the final measurement data, is highly sensitively dependent on the data. Despite that many researchers are dedicated to improve the solution of ill-posed problems, the recent results are still disappointing. In this dissertation, there are two methods adopted to deal with the direct problem of singular perturbed beam, and there are three methods adopted to deal with on the inverse problem of recovery force on the beam.
The singularly perturbed boundary value problems (SPBVPs) in Euler-Bernoulli beam is dominated by tension instead of rigidity. It contains a small perturbing parameter in its highest order derivative term. The small parameter is not considered as zero. Otherwise, the order of solution would be reduced. The weak-form integral equation method which contains the exponential and polynomial trial solutions weaken the governed beam equation and subsequently translate the differential operator to the continuous test functions. The collocation method is associated with the exponentially and polynomially fitted basis functions. It is different from the weak-form integral equation method. Instead of translating the differential operator to the test function, this method is adopted to directly satisfy the fourth-order ordinary differential equation at the collocation points. The force recovery problem refers to the inverse problem of the measured displacement data with noise, where the external force is unknown. If the measurement displacement data has a small disturbance, the result of the recovery external force will lead a serious consequence on error. The purpose of this dissertation is finding an appropriate approach to the inverse problem. The stable numerical differentiator to the fourth-order derivative method has the same concept of weak form integral equation method. The test functions which satisfy the boundary conditions are established. In addition, the trial external force functions are described by boundary conditions and shape functions. With these two features, the force expansion trial functions are flexible to recover the external force. The simple noniterative method is adopted the adjoint eigenfunctions as the test functions. Impressively, the test functions automatically satisfy the beam equation and the boundary conditions in one. With orthogonality of the adjoint eigenfunctions, a closed-form solution of the expansion coefficients can be determined. Consequently, the noniterative method to recover the unknown force at final time displacement data is obtained. The boundary functional method (BFM) is considering the work translation between force and displacement. With additional measurement data on the spatial force at the initial and final time, a series of spatial boundary functions are derived. Impressively, the boundary functions satisfy the governing equation and boundary conditions in one. Moreover, with the aid of the implicit time functions, the energy of work can be conservative for any boundary functions. In the case where all boundary functions are conservative, a linear space consisting of zero elements can be created. By solving the unknown coefficients of the spatial boundary function, we can reconstruct the external force. The more noise amplified, the more complicated the direct problems and inverse problems. In this dissertation, the adaptation of expansion terms on test function and expansion should be reconsidered with different types of the beam while the measurement is polluted with random noise. By comparing numerical computation and exact solution, this dissertation has deeply discussed all the adoption, and demonstrate the applications under the random noise in direct and inverse problems. | en |
| dc.description.provenance | Made available in DSpace on 2021-06-17T07:19:32Z (GMT). No. of bitstreams: 1 ntu-108-D03521004-1.pdf: 10156981 bytes, checksum: c429fda9a8e5b46bf403744984fda768 (MD5) Previous issue date: 2019 | en |
| dc.description.tableofcontents | 口試委員會審定書 i
Acknowledgments ii 致謝 iii 中文摘要 iv Abstract vi 1 Introduction 1 1.1 Problems description and motivations . . . . . . . . . . . . . . . . . . . 1 1.2 Literature review . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3 1.3 Organization of the dissertation . . . . . . . . . . . . . . . . . . . . . . . 5 2 Solving a Singular Beam Equation by Using a Weak-form Integral Equation Method (WFIEM) 8 2.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8 2.2 The governing ODE . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 9 2.3 A weak form method . . . . . . . . . . . . . . . . . . . . . . . . . . . . 9 2.4 Trial functions and test functions . . . . . . . . . . . . . . . . . . . . . . 10 2.5 Deriving linear system and determining the scales . . . . . . . . . . . . . 12 2.6 Numerical examples . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14 2.6.1 Example 1 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14 2.6.2 Example 2 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 16 2.6.3 Example 3 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 17 2.7 Conclusions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 18 3 A Collocation Method with Boundary Exponentially / Polynomially Fitted Trial Functions to Solve a Singularly Perturbed Beam 21 3.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 21 3.2 The Fourth-order Singularly Perturbed Beam . . . . . . . . . . . . . . . 22 3.3 Method 1 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 23 3.3.1 Fixed-end beam . . . . . . . . . . . . . . . . . . . . . . . . . . . 23 3.3.2 Simple beam . . . . . . . . . . . . . . . . . . . . . . . . . . . . 25 3.4 Method 2 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 25 3.4.1 Fixed-end beam . . . . . . . . . . . . . . . . . . . . . . . . . . . 25 3.4.2 Simple beam . . . . . . . . . . . . . . . . . . . . . . . . . . . . 26 3.5 Method 3 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 26 3.5.1 Fixed-end beam . . . . . . . . . . . . . . . . . . . . . . . . . . . 27 3.5.2 Simple beam . . . . . . . . . . . . . . . . . . . . . . . . . . . . 27 3.6 Examples . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 27 3.6.1 Fixed-end beam . . . . . . . . . . . . . . . . . . . . . . . . . . . 27 3.6.2 Simple beam . . . . . . . . . . . . . . . . . . . . . . . . . . . . 29 3.7 Conclusions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 30 4 A Stable Numerical Differentiator to the Fourth-order Derivative of Noisy Data 45 4.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 45 4.2 The first-order derivative method . . . . . . . . . . . . . . . . . . . . . . 46 4.3 The higher-order derivatives . . . . . . . . . . . . . . . . . . . . . . . . 49 4.4 Examples . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 50 4.4.1 Example 1 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 50 4.4.2 Example 2 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 52 4.5 Conclusions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 54 5 A Noniterative Method to Recover a Space-dependent Load on Euler-Bernoulli Beam Equation 83 5.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 83 5.2 Euler-Bernoulli Beam Theory . . . . . . . . . . . . . . . . . . . . . . . 84 5.2.1 Uniform and homogeneous boundary conditions of Euler-Bernoulli Beam . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 85 5.3 Green’s second identity . . . . . . . . . . . . . . . . . . . . . . . . . . . 85 5.4 Self-adjoint Operator . . . . . . . . . . . . . . . . . . . . . . . . . . . . 87 5.4.1 The adjoint Trefftz test function of v(x; t) . . . . . . . . . . . . . 88 5.5 Mode shape with different kinds of beams . . . . . . . . . . . . . . . . . 91 5.5.1 Simple beam . . . . . . . . . . . . . . . . . . . . . . . . . . . . 91 5.5.2 Cantilever beam . . . . . . . . . . . . . . . . . . . . . . . . . . 98 5.5.3 Hinged-clamped beam . . . . . . . . . . . . . . . . . . . . . . . 102 5.6 A Fictitious Time Integration Method (FTIM) . . . . . . . . . . . . . . . 104 5.7 Error Estimation and Adaptation of Terms . . . . . . . . . . . . . . . . . 106 5.8 Examples to Recover External Force H(x) on Simple Beam . . . . . . . . 107 5.8.1 Example 1 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 107 5.8.2 Example 2 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 128 5.8.3 Example 3 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 130 5.8.4 Example 4 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 132 5.8.5 Example 5 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 134 5.8.6 Example 6 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 136 5.9 Examples to Recover External Force H(x) on Cantilevered Beam . . . . . 138 5.9.1 Example 7 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 138 5.9.2 Example 8 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 140 5.10 Examples to Recover External Force H(x) on Hinged-Clamped Beam . . 143 5.10.1 Example 9 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 143 5.10.2 Example 10 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 145 5.11 Conclusions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 147 6 Identify Space-time Dependent Force on the Vibration of Euler-Bernoulli Beam by Using a Boundary Functional Method (BFM) 208 6.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 208 6.2 Inverse source problem . . . . . . . . . . . . . . . . . . . . . . . . . . . 209 6.3 Work functional of boundary functions . . . . . . . . . . . . . . . . . . . 211 6.4 Iterative algorithm to recover unknown force . . . . . . . . . . . . . . . . 214 6.5 Error Estimation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 216 6.6 Numerical examples of simple beam . . . . . . . . . . . . . . . . . . . . 217 6.6.1 Example 1 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 217 6.6.2 Example 2 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 218 6.6.3 Example 3 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 218 6.7 Numerical examples of cantilevered beam and two-end fixed beams . . . 219 6.7.1 Example 4 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 220 6.8 Numerical examples of two-end fixed beam . . . . . . . . . . . . . . . . 221 6.8.1 Example 5 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 221 6.8.2 Numerical examples of hinged-clamped beam . . . . . . . . . . . 222 6.8.3 Example 6 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 222 6.8.4 Example 7 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 223 6.8.5 Damped vibrating Euler-Bernoulli beam . . . . . . . . . . . . . . 223 6.8.6 Example 8 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 223 6.8.7 Example 9 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 224 6.9 Conclusions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 225 7 Conclusions and Future works 240 7.1 Conclusions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 240 7.2 Future Works . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 242 | |
| dc.language.iso | en | |
| dc.subject | 外力源恢復 | zh_TW |
| dc.subject | 伴隨特徵函數 | zh_TW |
| dc.subject | 非迭代法 | zh_TW |
| dc.subject | 奇異攝動梁 | zh_TW |
| dc.subject | 病態問題 | zh_TW |
| dc.subject | 邊界泛函法 | zh_TW |
| dc.subject | ill-posed problem | en |
| dc.subject | singular perturbed beam | en |
| dc.subject | force recovery | en |
| dc.subject | adjoint eigenfunctions | en |
| dc.subject | noniterative method | en |
| dc.subject | boundary functional method (BFM) | en |
| dc.title | 尤拉梁正反算問題之創新無網格計算方法研究 | zh_TW |
| dc.title | The Study of Novel Meshless Methods for Solving Direct and
Inverse Problems of Euler-Bernoulli Beam | en |
| dc.type | Thesis | |
| dc.date.schoolyear | 107-2 | |
| dc.description.degree | 博士 | |
| dc.contributor.oralexamcommittee | 張建仁,張致文,郭仲倫,陳寒濤 | |
| dc.subject.keyword | 病態問題,奇異攝動梁,外力源恢復,伴隨特徵函數,非迭代法,邊界泛函法, | zh_TW |
| dc.subject.keyword | ill-posed problem,singular perturbed beam,force recovery,adjoint eigenfunctions,noniterative method,boundary functional method (BFM), | en |
| dc.relation.page | 255 | |
| dc.identifier.doi | 10.6342/NTU201901057 | |
| dc.rights.note | 有償授權 | |
| dc.date.accepted | 2019-07-09 | |
| dc.contributor.author-college | 工學院 | zh_TW |
| dc.contributor.author-dept | 土木工程學研究所 | zh_TW |
| 顯示於系所單位: | 土木工程學系 | |
文件中的檔案:
| 檔案 | 大小 | 格式 | |
|---|---|---|---|
| ntu-108-1.pdf 未授權公開取用 | 9.92 MB | Adobe PDF |
系統中的文件,除了特別指名其著作權條款之外,均受到著作權保護,並且保留所有的權利。
