This paper deals with the nonlinear vibrations of a two hinged beam-column subjected to a harmonic forcing function of any space distribution. Vibration in the fundamental mode is investigated and regions of dynamic instability are found. The perturbation solution used is suitable for both strong an
The dynamic stability of a simply supported beam with additional discrete elements
β Scribed by Wojciech Sochacki
- Publisher
- Elsevier Science
- Year
- 2008
- Tongue
- English
- Weight
- 529 KB
- Volume
- 314
- Category
- Article
- ISSN
- 0022-460X
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β¦ Synopsis
The dynamic stability of a simply supported beam with additional discrete elements was investigated in the paper. Those elements were an elastic spring, a concentrated mass and an undamped harmonic oscillator connected to the beam. All the discrete elements could be mounted at any chosen position along the beam length. The beam was axially loaded by a harmonic force. The problem of dynamic stability was solved by applying the mode summation method. The obtained Mathieu equation allowed the influence of additional elements on the position of solutions on a stability chart to be analysed. The analysis relied on testing the influence of individual discrete elements on the value of coefficient b in the Mathieu equation. The research carried out showed that both the concentrated mass and oscillator mass had a destabilising effect (maximum in the middle position) on the investigated system. The rigidity of the support and the oscillator had an influence on an increase in the stability of the investigated system. An increase in the loading force, independently of the relation between the mass and rigidity of discrete elements, had an influence on the increase in coefficient b in the Mathieu equation (the less stable system). The considered beam is treated as a BernoulliβEuler beam in accordance with the small bending theory.
π SIMILAR VOLUMES
This paper deals with the linear dynamic response of a simply supported uniform beam under a moving load of constant magnitude and velocity by including the effect of its mass. Using a series solution for the dynamic deflection in terms of normal modes the individual and coupling effect of the mass