Abstract

In this paper, we revisit the capability of numerical approaches such as finite difference methods and finite element methods, in approximating exact one-dimensional continuous eigenvalue problems (such as lateral vibrations of a string, the axial or the torsional vibrations of a bar, and the buckling of elastic columns). The numerical methods analysed in this paper are converted into difference equations. Following a continualization procedure or the method of differential approximation, the difference operators are then expanded in differential operators via Taylor expansion or Pade approximants. Analogies between the finite numerical approaches and some equivalent enriched continuum are shown, using this continualization procedure. The finite difference methods (first-order or higher-order finite difference methods) are shown to behave as integral-based nonlocal media (or stress gradient media), while the finite element method is found to behave as gradient elasticity media (or strain gradient media). The length scale identification of each equivalent enriched continuum strongly depends on the order of the numerical method considered. For the finite difference methods, the length scale identification of the equivalent nonlocal medium depends on the static versus dynamic analysis, whereas this length scale appears to be independent of inertia effects for the finite element method. Some comparisons between the exact discrete eigenvalue problems and the approximated continuous ones show the efficiency of the continualization procedure. An equivalent enriched Rayleigh quotient can be defined for each numerical method: the integral-based nonlocal method gives a lower bound solution to the exact eigenvalue multiplier, whereas the gradient elasticity method furnishes an upper bound solution.

Highlights

  • The source of discreteness in mechanics or physics may come from the inherent nature of matter which is composed of a discrete number of local repetitive cells

  • We show that the rate of convergence is strongly dependent on the order of the finite discrete scheme: higher-order finite schemes lead to higher-order enriched constitutive laws with a higher convergence rate

  • A consequence of the nonlocal equivalent principle for the modeling of discrete systems is that the finite difference system can be efficiently approached by nonlocal continuum mechanics tools. As it is known in the case of nonlocal mechanics behaviors, this result confirms the lower bound solution of such approximate Finite Difference Methods, at least for homogeneous structures. We extend such a result for approximate Finite Element Methods using gradient elasticity constitutive law, which shows the upper bound solution of Finite Element results based on the workeenergy formulation

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Summary

Introduction

The source of discreteness in mechanics or physics may come from the inherent nature of matter which is composed of a discrete (or a finite) number of local repetitive cells. It has been recently argued that discrete elastic systems (including bending and shear interaction law) behave as nonlocal structural elements, in the context of the socalled continualization procedure (Wang et al, 2013; Challamel et al, 2014a; 2014b, 2014c, 2015c; Zhang et al, 2014a) This fundamental property has been shown on microstructured bending structural systems, and the induced nonlocality may be based on Eringen's classical model (Eringen, 1983) for the constitutive law. We have already shown for bending systems that finite difference formulation (or its analogical lattice physical system) has resemblance to nonlocal theory, whereas finite element formulation may have a strain gradient continuum analogy (see recently Challamel et al, 2015b for the analysis of beam vibrations). We first start from the string problem and investigate some column problems in buckling by both the finite difference and finite element methods

Discrete string problem
Finite difference method e buckling
Finite element method e buckling
Conclusions
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