2014
DOI: 10.1088/0266-5611/30/6/065008
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Uniqueness in the identification of asynchronous sources and damage in vibrating beams

Abstract: In this paper we analyze the problem of identification of the distribution of asynchronous vibration sources and rigidity perturbations in Euler-Bernoulli beams. Here it is proved that the displacement of a beam, even in an engineered continuous beam resting upon several supports, measured for an arbitrary small interval of time over an arbitrary small open set is enough for the unique determination of vibration sources. Using this result, we prove that perturbations in rigidity can be uniquely determined in a… Show more

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Cited by 22 publications
(21 citation statements)
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“…This contribution focuses on the determination of a unknown spatial load distribution f (x) from the final in time deflection in the nonhomogeneous Euler-Bernoulli beam and Kirchhoff-Love plate equations with arbitrary but separable source term. Other source identification problems for Euler-Bernoulli equations from boundary or final in time observations can be found in [12][13][14][15]20,24,32] and for the Kirchhoff-Love equation in [10]. In [32], using spectral theory, the point source a(x) is uniquely determined in the constant coefficient dynamic Euler-Bernoulli equationü + u = λ(t)a(x) where λ ∈ C 1 ([0, T ]) is given and x ∈ (0, 1).…”
Section: Literature Overviewmentioning
confidence: 99%
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“…This contribution focuses on the determination of a unknown spatial load distribution f (x) from the final in time deflection in the nonhomogeneous Euler-Bernoulli beam and Kirchhoff-Love plate equations with arbitrary but separable source term. Other source identification problems for Euler-Bernoulli equations from boundary or final in time observations can be found in [12][13][14][15]20,24,32] and for the Kirchhoff-Love equation in [10]. In [32], using spectral theory, the point source a(x) is uniquely determined in the constant coefficient dynamic Euler-Bernoulli equationü + u = λ(t)a(x) where λ ∈ C 1 ([0, T ]) is given and x ∈ (0, 1).…”
Section: Literature Overviewmentioning
confidence: 99%
“…The missing information is compensated by the following boundary measurements: respectively u (0, t) or u (0, t) for all t ∈ (0, T ). This source identification problem has been reconsidered in [20] for more general Euler-Bernoulli equation, which includes a constant damping and a constant traction force. An effective combination of the Lie-group adaptive method and the differential quadrature method is proposed in [24] to recover an unknown space and time dependent 3 load in a constant coefficient Euler-Bernoulli beam vibration equation.…”
Section: Literature Overviewmentioning
confidence: 99%
“…Then, we develop a closed‐form expansion coefficients method, which is a noniterative method, to recover the unknown function H ( x ) in Sfalse(x,tfalse)=Hfalse(xfalse)Ffalse(tfalse), where F ( t ) is a given function. The recovery of the spatial load H ( x ) has been studied by Nicaise and Zair, Hasanov, Kawano, and Hasanov and Baysal, assuming that F ( t ) is a given function of t . However, those methods are of iterative types.…”
Section: Closed‐form Expansion Coefficients Methodsmentioning
confidence: 99%
“…The force identification problems of beams have been studied in many research studies. [3][4][5][6][7][8] The parameter identification issue is a subclass of inverse problems, which was studied as the inverse spectral problems. [9][10][11] Besides, some researchers studied different models of the Euler-Bernoulli nanobeams [12][13][14][15][16][17][18][19][20][21] in a microscopic scale.…”
Section: Introductionmentioning
confidence: 99%
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