Abstract
In this work, we discuss the time optimal control of two dimensional convective Brinkman–Forchheimer (2D CBF) equations, which describe the motion of incompressible viscous fluid through a rigid, homogeneous, isotropic, porous medium. We establish Pontryagin’s maximum principle for the time optimal control of the 2D CBF equations.
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Notes
Since \({\mathbf {u}}\in \mathrm {C}([0,T];{\mathbb {V}})\cap \mathrm {L}^2(0,T;\mathrm {D}(\mathrm {A}))\) is the unique strong solution of the system (3.1) with the control \(\mathrm {U}\in \mathrm {L}^{\infty }(0,\infty ;{\mathbb {H}})\), we suppress the dependence of \({\mathbf {u}}(\cdot )\) in (4.2).
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Acknowledgements
M. T. Mohan would like to thank the Department of Science and Technology (DST), India for Innovation in Science Pursuit for Inspired Research (INSPIRE) Faculty Award (IFA17-MA110) and Indian Institute of Technology Roorkee, for providing stimulating scientific environment and resources. The author sincerely would like to thank the reviewers for their valuable comments and suggestions.
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Appendix A. Global Solvability of the Linearized System
Appendix A. Global Solvability of the Linearized System
In this section, we discuss the existence of a global strong solution to the linearized system (4.26). Let \({\mathbf {u}}(\cdot )\) be the unique strong solution to the system (A.3) with the control \(\mathrm {U}\) satisfying \({\mathbf {u}}\in \mathrm {C}([0,T];{\mathbb {V}})\cap \mathrm {L}^2(0,T;\mathrm {D}(\mathrm {A}))\). Then, we have the following result.
Theorem A.1
For \(\mathrm {U}\in \mathrm {L}^2(0,T;{\mathbb {H}})\), there exists a unique strong solution to the system
for a.e. \(t\in (0,T)\), satisfying
Proof
Using the standard Faedo-Galerkin technique, one can obtain the global solvability results. We only provide a-priori energy estimates satisfied by the system (A.1) and one can use Faedo-Galerkin approximation to make the calculations rigorous. Taking the inner product with \({\mathbf {z}}(\cdot )\) to the first equation in (A.1), we obtain
Integrating the above inequality from 0 to t, we find
for all \(t\in (0,T)\). An application of Gornwall’s inequality in (A.3) yields
for all \(t\in (0,T)\). Using (A.4) in (A.3), we get
Taking inner product with \(\mathrm {A}{\mathbf {z}}(\cdot )\) to the first equation in (A.1), we obtain
For \(r=2\), we estimate terms on the right hand side of the equality (A.6) using Hölder’s, Ladyzhenskaya’s, Agmon’s and Young’s inequalities as
Combining (A.7)-(A.10), substituting it in (A.6) and then integrating from 0 to t, we find
Applying Gronwall’s inequality in (A.11), we get
for all \(t\in [0,T]\). For \(r=3\), we need to estimate \(\beta |({\mathcal {C}}'({\mathbf {u}}){\mathbf {z}},\mathrm {A}{\mathbf {z}})|\) only. Using Hölder’s, Ladyzhenskaya’s, Agmon’s and Young’s inequalities, we estimate it as
In order to obtain time derivative estimates, we take the inner product with \(\partial _t{\mathbf {u}}(\cdot )\) with the first equation in (A.1) to find
We estimate \(|(\mathrm {B}({\mathbf {z}},{\mathbf {u}}),\partial _t{\mathbf {z}})|\) using (2.11) and Young inequality as
One can use the calculations similar to (A.7)-(A.10) and (A.13) to obtain \( \int _0^t\Vert \partial _t {\mathbf {u}}(s)\Vert _{{\mathbb {H}}}^2\mathrm {d}s\le C, \) for all \(t\in [0,T]\) and hence one can complete the Theorem. \(\square \)
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Mohan, M.T. The Time Optimal Control of Two Dimensional Convective Brinkman–Forchheimer Equations. Appl Math Optim 84, 3295–3338 (2021). https://doi.org/10.1007/s00245-021-09748-w
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DOI: https://doi.org/10.1007/s00245-021-09748-w
Keywords
- Convective Brinkman–Forchheimer equations
- Pontryagin’s maximum principle
- Porus medium
- Time optimal control