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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Online Access: | http://dx.doi.org/10.1080/23311835.2015.1021603 |
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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 |
work_keys_str_mv |
AT ludwigkohaupt twosidedboundsonthemeanvectorandcovariancematrixinlinearstochasticallyexcitedvibrationsystemswithapplicationofthedifferentialcalculusofnorms |
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