The stiffness matrix method

Structures ◽  
2000 ◽  
pp. 239-285
Author(s):  
M. S. Williams ◽  
J. D. Todd
2020 ◽  
Vol 143 (1) ◽  
Author(s):  
Masayuki Arai ◽  
Shoichi Kuroda ◽  
Kiyohiro Ito

Abstract Pipe systems have been widely used in industrial plants such as power stations. In these systems, the displacement and stress distributions often need to be predicted. Analytical and numerical methods, such as the finite element method (FEM), boundary element method (BEM), and frame structure method (FSM), are typically adopted to predict these distributions. The analytical methods, which can only be applied to problems with simple geometries and boundary conditions, are based on the Timoshenko beam theory. Both FEM and BEM can be applied to more complex problems, although this usually requires a stiffness matrix with a large number of degrees-of-freedom. In FSM, although the structure is modeled by a beam element, the stiffness matrix still becomes large; furthermore, the matrix size needed in FEM and BEM is also large. In this study, the transfer matrix method, which is simply referred to as TMM, is studied to effectively solve complex problems, such as a pipe structure under a small size stiffness matrix. The fundamental formula is extended to a static elastic-plastic problem. The efficiency and simplicity of this method in solving a space-curved pipe system that involves an elbow are demonstrated. The results are compared with those obtained by FEM to verify the performance of the method.


2019 ◽  
Vol 89 (9) ◽  
pp. 1923-1938
Author(s):  
Anvesh R. Nandyala ◽  
Ashish K. Darpe ◽  
Satinder P. Singh

2020 ◽  
Vol 77 ◽  
pp. 663-689 ◽  
Author(s):  
Shi-Jin Feng ◽  
Xiang-Hong Ding ◽  
Qi-Teng Zheng ◽  
Zhang-Long Chen ◽  
Dong-Mei Zhang

1995 ◽  
Vol 408 ◽  
Author(s):  
Y. E. Hsu ◽  
T. K. Chaki

AbstractA simulation of structure and motion of edge dislocations in ordered Ni3Al was performed by atomic stiffness matrix method. In this method the equilibrium positions of the atoms were obtained by solving a set of linear equations formed by a stiffness matrix, whose terms consisted of derivatives of the interaction potential of EAM (embedded atom method) type. The superpartial dislocations, separated by an antiphase boundary (APB) on (111), dissociated into Shockley partials with complex stacking faults (CSF) on (111) plane. The core structure, represented by the Burgers vector density distribution and iso-strain contours, changed under applied stresses as well as upon addition of boron. The separation between the superpartials changed with the addition of B and antisite Ni. As one Shockley partial moved out to the surface. a Shockley partial in the interior moved a large distance to join the lone one near the surface, leaving behind a long CSF strip. The decrease in the width of the APB upon addition of B and antisite Ni has been explained by a reduction of the strength of directional bonding between Ni and Al as well as by the dragging of B atmosphere by the superpartials.


1997 ◽  
Vol 63 (614) ◽  
pp. 3396-3401
Author(s):  
Keiji WATANABE ◽  
Kouetsu TAKANO ◽  
Osami MATSUSHITA ◽  
Masanori KITANO ◽  
Daisaku SATO

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