Dynamic Response of a Timoshenko Beam on an Elastic Foundation Subjected to Multiple Distributed Moving Loads

Authors

Alimi Adedowole

Department of Mathematical Sciences, Adekunle Ajasin University, Akungba-Akoko, Ondo State, Nigeria (Nigeria)

Sule Adekunle Jimoh

Department of Mathematical Sciences, Faculty of Natural and Applied Sciences, Achievers University, Owo, Ondo State, Nigeria (Nigeria)

Olawale Olanipekun Ajijola

Department of Mathematical Sciences, Adekunle Ajasin University, Akungba-Akoko, Ondo State, Nigeria (Nigeria)

Kayode Samuel Famuagun

Department of Mathematics, Adeyemi Federal University of Education, Ondo, Nigeria (Nigeria)

Abayomi Samuel Oke

Department of Mathematical Sciences, Adekunle Ajasin University, Akungba-Akoko, Ondo State, Nigeria (Nigeria)

Oluwaseun Olumide Okundalaye

Department of Mathematical Sciences, Adekunle Ajasin University, Akungba-Akoko, Ondo State, Nigeria (Nigeria)

Article Information

DOI: 10.51244/IJRSI.2026.1308000361

Subject Category: Mechanics

Volume/Issue: 13/8 | Page No: 5556-5576

Publication Timeline

Submitted: 2026-09-07

Accepted: 2026-09-12

Published: 2026-09-28

Abstract

This study develops and verifies a Galerkin formulation for the transient response of a simply supported Timoshenko beam on a Winkler foundation under two finite-length distributed loads. The model includes shear deformation, rotary inertia, a uniform tensile prestress, foundation stiffness, load spacing, travelling velocity, and constant or harmonic load amplitudes. Unlike a semi-infinite Heaviside step, each load is represented by the difference of two Heaviside functions, so that its physical footprint and entry and exit from the span are treated explicitly. Sine and cosine basis functions satisfying the simply supported conditions reduce the governing equations to independent two-degree-of-freedom modal systems. Laplace transformation and partial-fraction inversion give an explicit two-branch impulse-response solution; convolution with the projected moving loads then gives the final analytical displacement and rotation fields. The same retained-mode response is also evaluated by a state-transition convolution scheme, and the two forms agree to machine precision: both predict a peak midspan deflection of 2.9226547 mm at 2.400 s, with a maximum time-history difference of 3.27×10^(-13) mm. A systematic truncation study shows that 12 Galerkin modes differ from the 16-mode reference by only 0.023% in peak response and 0.012% in normalized root-mean-square error. An independent 100-element Timoshenko finite-element model gives 2.922 mm; the peak difference is 0.023%. Increasing the Winkler stiffness from 0 to 2.0 MN/m² reduces the peak response by 86.4%, while increasing tensile prestress from 0 to 120 MN produces a 42.9% reduction. Load spacing produces non-monotonic modal interference, and the velocity sweep gives a maximum dynamic amplification factor of 1.619 at 125 m/s for the selected parameters. Under undamped harmonic loading, excitation at the first flexural frequency produces the expected resonant growth during load passage. These verified results clarify the separate and interacting effects of foundation stiffness, tensile prestress, load magnitude, spacing, speed, and excitation frequency.

Keywords

Timoshenko beam; Winkler foundation; distributed moving load; Galerkin method; finite-element verification; dynamic amplification; resonance.

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References

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