2009
DOI: 10.1098/rspa.2009.0426
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A constrained eigenvalue problem and nodal and modal control of vibrating systems

Abstract: A constrained non-homogeneous linear eigenvalue problem is introduced. The application given to the problem is of finding the frequency and amplitudes of exciting forces that impose constraints on the configurations of vibratory modes. The scope of the problem is wider. It is shown that the problem may be transformed to a singular unsymmetric generalized eigenvalue problem. Depending on the given data the problem may have finite, infinite or empty spectrum. The solvability of the problem is analysed. Examples … Show more

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Cited by 3 publications
(4 citation statements)
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“…In this case, the uncertainty of the system synthesis problem arises: to build a modal controller, it is necessary to know the parameters of the reference channel с0 and с1, and to build the reference channel, it is necessary to know the characteristic polynomial of the in such a way that the inequality   (-а0,M/а1, M) holds [27][28][29]. Restricting ourselves to the case of negative real roots that is important for this problem, we prove the following theorem.…”
Section: Synthesis Methodsmentioning
confidence: 99%
“…In this case, the uncertainty of the system synthesis problem arises: to build a modal controller, it is necessary to know the parameters of the reference channel с0 and с1, and to build the reference channel, it is necessary to know the characteristic polynomial of the in such a way that the inequality   (-а0,M/а1, M) holds [27][28][29]. Restricting ourselves to the case of negative real roots that is important for this problem, we prove the following theorem.…”
Section: Synthesis Methodsmentioning
confidence: 99%
“…In an attempt to generalize such an approach to allow for higher order formulas, and differential constraints which are arbitrary in form and number, we might consider the problem [15],…”
Section: Eigenfunctions Of Linear Differential Operatorsmentioning
confidence: 99%
“…with the additional requirement ∥⃗ y∥ 2 2 = 1. While this does appear to be a standard problem of linear algebra, the fact is that while it may be a consistent discretization, it may yield a grand total of zero eigenvalueeigenvector pairs [15]. The formulation of the discretized eigenfunction problem in Eqn.…”
Section: Eigenfunctions Of Linear Differential Operatorsmentioning
confidence: 99%
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