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Titlebook: Control of Higher–Dimensional PDEs; Flatness and Backste Thomas Meurer Book 2013 Springer-Verlag Berlin Heidelberg 2013 Backstepping.Contro

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31#
發(fā)表于 2025-3-27 00:16:29 | 只看該作者
32#
發(fā)表于 2025-3-27 03:33:51 | 只看該作者
33#
發(fā)表于 2025-3-27 09:00:18 | 只看該作者
Alexandria: Hochburg der Wissenschaftene applied by considering a suitable control volume, which is either fixed in space or moving within a fluid. With this, selected application examples and the related control problems are introduced and briefly discussed towards their analysis in subsequent chapters.
34#
發(fā)表于 2025-3-27 13:14:01 | 只看該作者
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發(fā)表于 2025-3-27 15:53:04 | 只看該作者
36#
發(fā)表于 2025-3-27 21:18:25 | 只看該作者
Alexandria: Hochburg der Wissenschaftenion–reaction systems (Chapters 2 and 3) or so–called biharmonic Petrowski systems (Chapter 4) defined on bounded higher–dimensional domains. This enables a rigorous formulation of the subsequently analyzed control problems.
37#
發(fā)表于 2025-3-28 00:50:48 | 只看該作者
https://doi.org/10.1007/978-3-658-44118-0 and feedback control design. The dynamic system properties are thereby determined based on the eigenvalue distribution and the respective set of eigenvectors. For infinite–dimensional systems governed by PDEs certain restrictions apply, which are in particular related to the possible existence of c
38#
發(fā)表于 2025-3-28 04:31:21 | 只看該作者
https://doi.org/10.1007/978-3-658-44216-3oblems. In the following a design technique is presented for boundary controlled scalar diffusion–convection–reaction systems with general spatially and time varying parameters defined on a 1 ≤ .–dimensional parallelepipedon. For this, it is assumed that the input relating state and gradient in a ge
39#
發(fā)表于 2025-3-28 07:01:42 | 只看該作者
40#
發(fā)表于 2025-3-28 10:40:31 | 只看該作者
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