The dynamic response of a spinning Timoshenko beam with general boundary conditions and subjected to a moving load is solved analytically for the first time. Solution of the problem is achieved by formulating the spinning Timoshenko beams as a non-self-adjoint system. To compute the system dynamic response using the modal analysis technique, it is necessary to determine the eigenquantities of both the original and adjoint systems. In order to fix the adjoint eigenvectors relative to the eigenvectors of the original system, the biorthonormality conditions are invoked. Responses for the four classical boundary conditions which do not involve rigidbody motions are illustrated. To ensure the validity of the method, these results are compared with those from Euler-Bernoulli and Rayieigh beam theories. Numerical simulations are performed to study the influence of the four boundary conditions on selected system parameters.
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March 1994
Research Papers
Dynamic Response of a Spinning Timoshenko Beam With General Boundary Conditions and Subjected to a Moving Load
J. W.-Z. Zu,
J. W.-Z. Zu
Department of Mechanical and Industrial Engineering, University of Manitoba, Winnipeg, Manitoba, R3T 2N2 Canada
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R. P. S. Han
R. P. S. Han
Department of Mechanical and Industrial Engineering, University of Manitoba, Winnipeg, Manitoba, R3T 2N2 Canada
Search for other works by this author on:
J. W.-Z. Zu
Department of Mechanical and Industrial Engineering, University of Manitoba, Winnipeg, Manitoba, R3T 2N2 Canada
R. P. S. Han
Department of Mechanical and Industrial Engineering, University of Manitoba, Winnipeg, Manitoba, R3T 2N2 Canada
J. Appl. Mech. Mar 1994, 61(1): 152-160 (9 pages)
Published Online: March 1, 1994
Article history
Received:
December 16, 1991
Revised:
March 8, 1993
Online:
March 31, 2008
Citation
Zu, J. W., and Han, R. P. S. (March 1, 1994). "Dynamic Response of a Spinning Timoshenko Beam With General Boundary Conditions and Subjected to a Moving Load." ASME. J. Appl. Mech. March 1994; 61(1): 152–160. https://doi.org/10.1115/1.2901390
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