Two-sided bounds on the mean vector and covariance matrix in linear stochastically excited vibration systems with application of the differential calculus of norms

For a linear stochastic vibration model in state-space form, $ \dot{x}(t) = A x(t)+b(t), \, x(0)=x_0, $ with system matrix A and white noise excitation $ b(t) $, under certain conditions, the solution $ x(t) $ is a random vector that can be completely described by its mean vector, $ m_x(t):=m_{x(t)}...

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Main Author: Ludwig Kohaupt
Format: Article
Language:English
Published: Taylor & Francis Group 2015-12-01
Series:Cogent Mathematics
Subjects:
Online Access:http://dx.doi.org/10.1080/23311835.2015.1021603
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spelling doaj-6b71f5aa7ddf4da9859eeb8e3aabb5a12020-11-24T21:46:48ZengTaylor & Francis GroupCogent Mathematics2331-18352015-12-012110.1080/23311835.2015.10216031021603Two-sided bounds on the mean vector and covariance matrix in linear stochastically excited vibration systems with application of the differential calculus of normsLudwig Kohaupt0Beuth University of Technology BerlinFor a linear stochastic vibration model in state-space form, $ \dot{x}(t) = A x(t)+b(t), \, x(0)=x_0, $ with system matrix A and white noise excitation $ b(t) $, under certain conditions, the solution $ x(t) $ is a random vector that can be completely described by its mean vector, $ m_x(t):=m_{x(t)} $, and its covariance matrix, $ P_x(t):=P_{x(t)} $. If matrix $ A $ is asymptotically stable, then $ m_x(t) \rightarrow 0 \, (t \rightarrow \infty ) $ and $ P_x(t) \rightarrow P \, (t \rightarrow \infty ) $, where $ P $ is a positive (semi-)definite matrix. As the main new points, in this paper, we derive two-sided bounds on $ \Vert m_x(t)\Vert _2 $ and $ \Vert P_x(t)- P\Vert _2 $ as well as formulas for the right norm derivatives $ D_+^k \Vert P_x(t)- P\Vert _2, \, k=0,1,2 $, and apply these results to the computation of the best constants in the two-sided bounds. The obtained results are of special interest to applied mathematicians and engineers.http://dx.doi.org/10.1080/23311835.2015.1021603linear stochastic vibration system excited by white noisemean vectorcovariance matrixtwo-sided boundsdifferential calculus of norms
collection DOAJ
language English
format Article
sources DOAJ
author Ludwig Kohaupt
spellingShingle Ludwig Kohaupt
Two-sided bounds on the mean vector and covariance matrix in linear stochastically excited vibration systems with application of the differential calculus of norms
Cogent Mathematics
linear stochastic vibration system excited by white noise
mean vector
covariance matrix
two-sided bounds
differential calculus of norms
author_facet Ludwig Kohaupt
author_sort Ludwig Kohaupt
title Two-sided bounds on the mean vector and covariance matrix in linear stochastically excited vibration systems with application of the differential calculus of norms
title_short Two-sided bounds on the mean vector and covariance matrix in linear stochastically excited vibration systems with application of the differential calculus of norms
title_full Two-sided bounds on the mean vector and covariance matrix in linear stochastically excited vibration systems with application of the differential calculus of norms
title_fullStr Two-sided bounds on the mean vector and covariance matrix in linear stochastically excited vibration systems with application of the differential calculus of norms
title_full_unstemmed Two-sided bounds on the mean vector and covariance matrix in linear stochastically excited vibration systems with application of the differential calculus of norms
title_sort two-sided bounds on the mean vector and covariance matrix in linear stochastically excited vibration systems with application of the differential calculus of norms
publisher Taylor & Francis Group
series Cogent Mathematics
issn 2331-1835
publishDate 2015-12-01
description For a linear stochastic vibration model in state-space form, $ \dot{x}(t) = A x(t)+b(t), \, x(0)=x_0, $ with system matrix A and white noise excitation $ b(t) $, under certain conditions, the solution $ x(t) $ is a random vector that can be completely described by its mean vector, $ m_x(t):=m_{x(t)} $, and its covariance matrix, $ P_x(t):=P_{x(t)} $. If matrix $ A $ is asymptotically stable, then $ m_x(t) \rightarrow 0 \, (t \rightarrow \infty ) $ and $ P_x(t) \rightarrow P \, (t \rightarrow \infty ) $, where $ P $ is a positive (semi-)definite matrix. As the main new points, in this paper, we derive two-sided bounds on $ \Vert m_x(t)\Vert _2 $ and $ \Vert P_x(t)- P\Vert _2 $ as well as formulas for the right norm derivatives $ D_+^k \Vert P_x(t)- P\Vert _2, \, k=0,1,2 $, and apply these results to the computation of the best constants in the two-sided bounds. The obtained results are of special interest to applied mathematicians and engineers.
topic linear stochastic vibration system excited by white noise
mean vector
covariance matrix
two-sided bounds
differential calculus of norms
url http://dx.doi.org/10.1080/23311835.2015.1021603
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