An exact solution of truss vibration problems
The Elements by a System of Transfer equations (EST) method offers exact solutions to various vibration problems of trusses, beams, and frames. The method can be regarded as an improved or modified transfer matrix method. Using the EST method, the roundoff errors generated by multiplying transfer ar...
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doaj-7196ec07114e415aa6f1d57d46310b992020-11-24T21:22:12ZengEstonian Academy PublishersProceedings of the Estonian Academy of Sciences1736-60461736-75302019-05-0168324426310.3176/proc.2019.3.0410.3176/proc.2019.3.04An exact solution of truss vibration problemsAndres Lahe0Andres Braunbrück1Aleksander Klauson2Department of Civil Engineering and Architecture, Tallinn University of Technology, Ehitajate tee 5; Corresponding authors, Andres.Lahe@ttu.eeDepartment of Civil Engineering and Architecture, Tallinn University of Technology, Ehitajate tee 5; Corresponding authors, andres@ioc.eeDepartment of Civil Engineering and Architecture, Tallinn University of Technology, Ehitajate tee 5The Elements by a System of Transfer equations (EST) method offers exact solutions to various vibration problems of trusses, beams, and frames. The method can be regarded as an improved or modified transfer matrix method. Using the EST method, the roundoff errors generated by multiplying transfer arrays are avoided. It is assumed that the bars of trusses are connected by frictionless joints. Longitudinal vibration of a truss bar is described by a differential equation. In a direction perpendicular to the longitudinal axis, no bending can occur. In a transverse direction the rigid bar displacements vary linearly. The rigid bar rotational moment of inertia is taken into account. The transfer equations for the truss bar are presented. The transverse displacements at the joint (node) of an elastic and a rigid bar are equal. The essential boundary conditions at joints for the differential equation are the compatibility conditions of the displacements of truss elements. The natural boundary conditions at joints are the equilibrium equations of longitudinal elastic forces and transverse inertial forces of rigid bars.http://www.kirj.ee/public/proceedings_pdf/2019/issue_3/proc-2019-3-244-263.pdftruss bar vibrationtransfer equationsessential boundary conditions at jointsnatural boundary conditions at jointsmaster–slave connectivitytransverse inertial forces. |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Andres Lahe Andres Braunbrück Aleksander Klauson |
spellingShingle |
Andres Lahe Andres Braunbrück Aleksander Klauson An exact solution of truss vibration problems Proceedings of the Estonian Academy of Sciences truss bar vibration transfer equations essential boundary conditions at joints natural boundary conditions at joints master–slave connectivity transverse inertial forces. |
author_facet |
Andres Lahe Andres Braunbrück Aleksander Klauson |
author_sort |
Andres Lahe |
title |
An exact solution of truss vibration problems |
title_short |
An exact solution of truss vibration problems |
title_full |
An exact solution of truss vibration problems |
title_fullStr |
An exact solution of truss vibration problems |
title_full_unstemmed |
An exact solution of truss vibration problems |
title_sort |
exact solution of truss vibration problems |
publisher |
Estonian Academy Publishers |
series |
Proceedings of the Estonian Academy of Sciences |
issn |
1736-6046 1736-7530 |
publishDate |
2019-05-01 |
description |
The Elements by a System of Transfer equations (EST) method offers exact solutions to various vibration problems of trusses, beams, and frames. The method can be regarded as an improved or modified transfer matrix method. Using the EST method, the roundoff errors generated by multiplying transfer arrays are avoided. It is assumed that the bars of trusses are connected by frictionless joints. Longitudinal vibration of a truss bar is described by a differential equation. In a direction perpendicular to the longitudinal axis, no bending can occur. In a transverse direction the rigid bar displacements vary linearly. The rigid bar rotational moment of inertia is taken into account. The transfer equations for the truss bar are presented. The transverse displacements at the joint (node) of an elastic and a rigid bar are equal. The essential boundary conditions at joints for the differential equation are the compatibility conditions of the displacements of truss elements. The natural boundary conditions at joints are the equilibrium equations of longitudinal elastic forces and transverse inertial forces of rigid bars. |
topic |
truss bar vibration transfer equations essential boundary conditions at joints natural boundary conditions at joints master–slave connectivity transverse inertial forces. |
url |
http://www.kirj.ee/public/proceedings_pdf/2019/issue_3/proc-2019-3-244-263.pdf |
work_keys_str_mv |
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1725996992237142016 |