Research Papers

A Screw Theory of Timoshenko Beams

[+] Author and Article Information
J. M. Selig

Faculty of Business, Computing and Information Management, London South Bank University, London SE1 0AA, UKseligjm@lsbu.ac.uk

Xilun Ding

Robotics Research Institute, Beijing University of Aeronautics and Astronautics, Beijing 100083, P. R. China

J. Appl. Mech 76(3), 031003 (Mar 05, 2009) (7 pages) doi:10.1115/1.3063630 History: Received December 18, 2006; Revised October 02, 2008; Published March 05, 2009

In this work, the classic theory of Timoshenko beams is revisited using screw theory. The theory of screws is familiar from robotics and the theory of mechanisms. A key feature of the screw theory is that translations and rotations are treated on an equal footing and here this means that bending, torsion, and extensions can all be considered together in a particularly simple manner. By combining forces and torques into a six-dimensional vector called a wrench, Hooke’s law for the Timoshenko beam can be written in a very simple form. From here simple expressions can be found for the kinetic and potential energy densities of the beam. Hence equations of motion for small vibrations of the beam can be easily derived. The screw theory also leads to a new understanding of the boundary conditions for beams. It is demonstrated that simple boundary conditions are closely related to mechanical joints. In order to set up the boundary conditions for a beam attached to a joint, a system of wrenches dual to the screws representing the freedoms of the joint must be found. Finally, a screw version of the Rayleigh–Ritz numerical method is introduced. An example is investigated in which the boundary conditions on the beam lead to vibrational modes of the beam involving bending, torsion, and extension at the same time.

Copyright © 2009 by American Society of Mechanical Engineers
Your Session has timed out. Please sign back in to continue.



Grahic Jump Location
Figure 1

Coordinate frames along the beam

Grahic Jump Location
Figure 2

The first three modes shapes. The thick lines at the ends represent direction of the joint axes.



Some tools below are only available to our subscribers or users with an online account.

Related Content

Customize your page view by dragging and repositioning the boxes below.

Related Journal Articles
Related eBook Content
Topic Collections

Sorry! You do not have access to this content. For assistance or to subscribe, please contact us:

  • TELEPHONE: 1-800-843-2763 (Toll-free in the USA)
  • EMAIL: asmedigitalcollection@asme.org
Sign In