Letter to the editorOn the governing equations for vibration and stability of a Timoshenko beam: Hamilton's principle
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Cited by (42)
Stability of Timoshenko beams with frequency and initial stress dependent nonlocal parameters
2019, Archives of Civil and Mechanical EngineeringCitation Excerpt :Sundaramaiah and Venkateswara Rao [8], using the finite element method, determined critical loads for cantilever Timoshenko beams resting on an elastic foundation and loaded with follower forces. Sato [9] on the basis of Hamilton's principle derived equations describing the vibration of the Timoshenko beam loaded with an axial force and a lateral force. Ruta [10] analysed, using Chebyshev polynomials, the stability of nonprismatic beams and frames based on the Timoshenko theory.
Critical contrasting of three versions of vibrating Bresse–Timoshenko beam with a crack
2017, International Journal of Solids and StructuresExact free vibration analysis for mechanical system composed of Timoshenko beams with intermediate eccentric rigid body on elastic supports: An experimental and analytical investigation
2017, Mechanical Systems and Signal ProcessingCitation Excerpt :Huang [2] investigated the frequency equations and normal modes of free flexural vibrations of uniform beams including the effect of shear deformation and rotary inertia for classical end conditions. Sato [3] investigated the governing equations for vibration and stability of a Timoshenko beam subjected to an axial load using Hamilton’s principle. Farghaly [4] derived an exact frequency equation for uniform cantilever Bernoulli–Euler beam with an elastically mounted non concentrated tip mass.
Exact free vibration of multi-step Timoshenko beam system with several attachments
2016, Mechanical Systems and Signal ProcessingCitation Excerpt :Effects of such support flexibilities on the natural frequencies of flexural vibration of beams have been studied and presented in Blevins and Plunkett [4]. The differential equation of motion, based on Timoshenko beam element with sides not perpendicular to the deflected axis of beam and with axial force, has been introduced with axial force term by Sato [5]. Farghaly [6] derived an exact frequency equation for uniform cantilever Bernoulli–Euler beam with an elastically mounted nonconcetrated tip mass.