2014
DOI: 10.1016/j.cam.2012.11.026
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Quadratic inverse eigenvalue problem for damped gyroscopic systems

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Cited by 12 publications
(9 citation statements)
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“…Therefore, it follows that if (38) holds; then, (40) holds for every λ. Additionally, note that λ ∈ R + since D d > 0; hence, the spectrum of A is positive. Remark 7: Another convenient inequality for implementation purposes corresponds to 2 .…”
Section: On the Behavior Of The Closed-loop System Near The Equilibriummentioning
confidence: 97%
See 1 more Smart Citation
“…Therefore, it follows that if (38) holds; then, (40) holds for every λ. Additionally, note that λ ∈ R + since D d > 0; hence, the spectrum of A is positive. Remark 7: Another convenient inequality for implementation purposes corresponds to 2 .…”
Section: On the Behavior Of The Closed-loop System Near The Equilibriummentioning
confidence: 97%
“…In the following proposition, we exploit this tuple for assigning a "worst" (or upper bound) value for the rise time of systems that verify (38). To this end, we define the rise time as the time taken by the system to reach 98% of its steady state value.…”
Section: On the Behavior Of The Closed-loop System Near The Equilibriummentioning
confidence: 99%
“…where , , , , 1 , 1 , 1 , 1 , , , , and are, respectively, given by (23), (25), (27), (28), and (29), with s, t ∈ R being arbitrary vectors.…”
Section: The Solution Of Problemmentioning
confidence: 99%
“…It is observed that model updating problems for linear viscously damped elastic systems (or gyroscopic systems) have been considered by many authors [21][22][23][24][25][26][27][28][29]. However, problems for updating hysteretic damping models have not got enough attention in these years.…”
Section: Introductionmentioning
confidence: 99%
“…Inverse eigenvalue problems with Jacobi, Toeplitz, and nonnegative matrices occur in a large number of applications ranging from applied mechanics and physics to numerical analysis, for more details see . The eigenvalues λ and the corresponding eigenvectors x of the quadratic eigenvalue problem Q ( λ ) x : = ( λ 2 A + λ B + C ) x = 0 can interpret the dynamical behavior of the second order differential system Ax¨false(tfalse)+Btrueẋfalse(tfalse)+Cxfalse(tfalse)=ffalse(tfalse) with mass, damping and stiffness matrices which arises in the acoustic simulation of poro‐elastic materials, the elastic deformation of anisotropic materials, and finite element discretization in structural analysis . The quadratic inverse eigenvalue problem is to construct the matrices A , B , and C such that the quadratic eigenvalue problem holds, that is, for given X=false(x1,x2,,xnfalse)Rn×m and normalΛ=diagfalse(λ1,λ2,,λmfalse)Rm×m, we find A , B , C ∈ R n × n such that A X Λ 2 + B X Λ + C X = 0.…”
Section: Introductionmentioning
confidence: 99%