Transverse vibration of an axially compressed bar with dry friction at its ends

The transverse vibration of a bar is studied by applying the Bernoulli-Euler beam theory. The bar is placed between the platens of a hydraulic press that applies compressive stress. When the bar vibrates, its ends slide over the platens with dry friction. Boundary conditions appropriate to the exist...

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Detalles Bibliográficos
Autores: Nieves Pavón, Francisco José, Bayón Rojo, Ana Isabel, Salazar Bloise, Félix José, Gascón Latasa, Francisco
Tipo de recurso: artículo
Estado:Versión publicada
Fecha de publicación:2025
País:España
Institución:Universidad de Sevilla (US)
Repositorio:idUS. Depósito de Investigación de la Universidad de Sevilla
OAI Identifier:oai:idus.us.es:11441/175047
Acceso en línea:https://hdl.handle.net/11441/175047
https://doi.org/10.1016/j.finmec.2025.100320
Access Level:acceso abierto
Palabra clave:Bernoulli-Euler beam theory
Bar with sliding ends
Transverse vibration
Axially compressed bar
Dry friction
Descripción
Sumario:The transverse vibration of a bar is studied by applying the Bernoulli-Euler beam theory. The bar is placed between the platens of a hydraulic press that applies compressive stress. When the bar vibrates, its ends slide over the platens with dry friction. Boundary conditions appropriate to the existence of friction are proposed. Once the homogeneous equation of motion is solved analytically, a particular solution is obtained through elementary trigonometric series. The sum of these solutions provides the general solution that shows the movement of all the bar points. The movement is divided into successive stages. The displacement of the bar points as a function of time is calculated numerically. It is demonstrated that there is a sudden change in the shape of vibrating when a specific number of semi-oscillations is reached, going from a behaviour of sliding ends to another of fixed ends. Criteria are proposed to estimate the circumstances in which the partial stop of the vibration occurs, as well as a change in the vibration mode and its frequency.