1983
DOI: 10.1002/nme.1620190310
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Damped second‐order Rayleigh‐Timoshenko beam vibration in space—an exact complex dynamic member stiffness matrix

Abstract: SUMMARYA uniform linear beam in a uniform linear ambient medium is studied. The beam performs stationary harmonic damped nonsynchronous space vibration in simultaneous tension, torsion, bending and shear in the presence of a large static axial load. Hysteretic and viscous dampings of the beam material and ambient medium are considered. Generalized complex KolouSek functions are derived. A 12 x 12 complex symmetric stiffness matrix is established for a supported beam member excited at its ends by prescribed har… Show more

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Cited by 77 publications
(19 citation statements)
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“…Nowadays many types of finite element for this type of beam model have been proposed. Lunde´n and Å kesson [3] have derived an element from the homogeneous solution of the modal equation of a corresponding beam. The interpolation functions of this element are dependent on the frequency, and thus both the eigenvalues and the eigenmodes of the discretized equation are calculated through non-linear eigenvalue analysis.…”
Section: Introductionmentioning
confidence: 99%
“…Nowadays many types of finite element for this type of beam model have been proposed. Lunde´n and Å kesson [3] have derived an element from the homogeneous solution of the modal equation of a corresponding beam. The interpolation functions of this element are dependent on the frequency, and thus both the eigenvalues and the eigenmodes of the discretized equation are calculated through non-linear eigenvalue analysis.…”
Section: Introductionmentioning
confidence: 99%
“…Na osnovu rešenja problema slobodnih vibracija pravog grednog nosača, koje postoji u zatvorenom obliku, izvedene su dinamičke matrice krutosti po Euler-Bernoulli-jevoj i Timoshenkoovoj teoriji [1][2][3][4]. Casimir [5] je odredio dinamičku matricu krutosti zakrivljene grede, pri čemu je rešenje diferencijalne jednačine odredio numerički.…”
Section: Introductionunclassified
“…Based on the closed form solution of the free vibration of a straight beam, the dynamic stiffness matrix according to the Euler-Bernoulli and Timoshenko beam theory was formulated [1][2][3][4]. Casimir [5] developed the dynamic stiffness matrix of a curved beam, whereby the differential equations were solved numerically.…”
Section: Introductionmentioning
confidence: 99%
“…Although this method has been in existence for a long time under the name of the dynamic stiffness method, its use was limited to simple vibration studies. This method is a merger of the direct dynamic stiffness method [33][34][35] and the finite element displacement method [36]. Elements are formulated and assembled as in the standard FEM while the base functions are the frequency dependent local solutions of the equations of motion.…”
Section: Introductionmentioning
confidence: 99%