Abstract

The present contribution describes a numerical technique devoted to the nonsmooth modal analysis (natural frequencies and mode shapes) of a non-internally resonant elastic bar of length L subject to a Robin condition at x = 0 and a frictionless unilateral contact condition at x = L. When contact is ignored, the system of interest exhibits non-commensurate linear natural frequencies, which is a critical feature in this study. The nonsmooth modes of vibration are defined as one-parameter continuous families of nonsmooth periodic orbits satisfying the local equation together with the boundary conditions. In order to find a few of the above families, the unknown displacement is first expressed using the well-known d’Alembert’s solution incorporating the Robin boundary condition at x = 0. The unilateral contact constraint at x = L is reduced to a conditional switch between Neumann (open gap) and Dirichlet (closed gap) boundary conditions. Finally, T-periodicity is enforced. It is also assumed that only one contact switch occurs every period. The above system of equations is numerically solved for through a simultaneous discretization of the space and time domains, which yields a set of equations and inequations in terms of discrete displacements and velocities. The proposed approach is non-dispersive, non-dissipative and accurately captures the propagation of waves with discontinuous fronts, which is essential for the computation of periodic motions in this study. Results indicate that in contrast to its linear counterpart (bar without contact constraints) where modal motions are sinusoidal functions “uncoupled” in space and time, the system of interest features nonsmooth periodic displacements that are intricate piecewise sinusoidal functions in space and time. Moreover, the corresponding frequency-energy “nonlinear” spectrum shows backbone curves of the hardening type. It is also shown that nonsmooth modal analysis is capable of efficiently predicting vibratory resonances when the system is periodically forced. The pre-stressed and initially grazing bar configurations are also briefly discussed.

Highlights

  • Techniques traditionally employed for nonlinear modal analysis require a certain degree of smoothness in the nonlinearities [12] and fail for systems with nonsmooth nonlinearities such as unilateral contact constraints

  • The complete internal resonance condition is annihilated by changing the boundary condition (BC) at x D 0 from Dirichlet type u.0; t / D 0 to a Robin type @xu.0; t / ̨u.0; t / D 0 which reflects that the elastic bar is connected to a rigid support through a simple linear spring1

  • It clearly resembles the corresponding nonsmooth modes (NSMs) motion, see Fig. 3. This forced solution seems to be identical to the autonomous oscillation, its free phase is not symmetric with respect to a time axis located in the middle of the free phase. This contribution targeted the nonsmooth modal analysis of a non-internally resonant bar through a numerical strategy based on simultaneous space-time discretization of the travelling-wave solution

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Summary

Introduction

The concept of linear modes (natural frequencies and mode shapes) is a widely studied subject in the field of structural dynamics [7]. Modal analysis of nonsmooth mechanical systems, called nonsmooth modal analysis, has been recently proposed for a finite elastic bar of length L subject to a Dirichlet boundary condition at x D 0 and a unilateral contact constraint at x D L [13]. This system satisfies a complete internal resonance condition, i.e. all linear natural frequencies are commensurate with the first one, which has drastic consequences on the nonlinear modal response. A numerical scheme based on the simultaneous discretization of the space and time domains is employed and the nonsmooth modes of vibration are constructed

Non-internally resonant elastic bar
Periodic solutions and Nonsmooth Modal Analysis
Numerical Scheme
Spectrum of nonsmooth vibration
Response to periodic external forcing
Conclusions

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