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IssuesArchive of Issues2002-5pp.115-121

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F. M. Detinko, "Follower load and the lateral buckling stability of a beam," Mech. Solids. 37 (5), 115-121 (2002)
Year 2002 Volume 37 Number 5 Pages 115-121
Title Follower load and the lateral buckling stability of a beam
Author(s) F. M. Detinko (USA)
Abstract The lateral buckling stability of a beam has been the subject matter of numerous studies (e.g., [1-3]). In the present paper, the lateral buckling stability is investigated for a beam of a solid cross-section under the action of a follower force in the plane of its greatest rigidity. For example, of this type is the load created by a jet engine fixed to the wing of an aircraft.

A solution of the problem of plane bending is represented in closed form, and then equations of the perturbed motion of the beam are constructed. The linearized equation of the perturbed motion can be divided into two groups, one governing flexural-and-torsional vibrations leading the beam out of the plane of the undeformed state and the other governing flexural vibrations in that plane. The eigenvalues of these equations with variable coefficients are found by the finite-element method.

It is found that the behavior of eigenvalues corresponding to flexural-and-torsional vibrations of a beam with rectangular cross-section can be of two different types. If the ratio of the sides of the rectangle satisfies the inequality β≤0.65, the variation in the eigenvalues as the load changes is the same as in the problem of [4, 5]. Namely, if there is no damping and the load is small, the eigenvalues are purely imaginary; when the load p reaches a value p=p*, the two lowest eigenvalues joint together, and for p>p*, there appear eigenvalues with small real parts. The value p* is the critical load upper bound.

For β>0.65, a large positive eigenvalue appears on the lateral buckling stability boundary. As the load increases beyond the critical value, this eigenvalue decreases, then attains a minimum and increases again.

For β<0.48, the critical value for the load of constant direction is less than the critical value for the follower load, however, for β>0.48 the former critical value exceeds the latter one.

Everywhere in this paper, we deal with Lyapunov stability in small.
References
1.  S. P. Timoshenko, Stability of Elastic Systems [Russian translation], Gostekhizdat, Moscow, 1955.
2.  D. H. Hodges and D. A. Peters, "On the lateral buckling of uniform slender cantilever beams," Intern J. Solids and Structures, Vol. 11, No. 12, pp. 1269-1280, 1975.
3.  Yong Lin Pi and N. S. Trahair, "Prebuckling deflections and lateral buckling, I. Theory," J. Struct. Eng., Vol. 118, No. 11, pp. 2949-2966, 1992.
4.  V. V. Bolotin, Nonconservative Problems in the Theory of Elastic Stability [in Russian], Fizmatgiz, Moscow, 1961.
5.  Ya. G. Panovko and I. I. Gubanova, Stability and Vibrations of Elastic Systems [in Russian], Nauka, Moscow, 1987.
6.  K. F. Chernykh, Nonlinear Theory of Elasticity in Machine Design [in Russian], Mashinostroenie, Leningrad, 1986.
7.  A. E. H. Love, A Treatise on the Mathematical Theory of Elasticity [Russian translation], ONTI, Moscow, Leningrad, 1935.
8.  G. G. Denisova and V. V. Novikov, "On the stability of a beam loaded by a "follower" force," Izv. AN SSSR. MTT [Mechanics of Solids], No. 1, pp. 150-154, 1975.
Received 11 May 2000
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