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Numerical Heat Transfer, Part B: Fundamentals
An International Journal of Computation and Methodology
Volume 70, 2016 - Issue 1
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Original Articles

Optimal flow control using a POD-based reduced-order model

, &
Pages 1-24 | Received 05 Oct 2015, Accepted 20 Feb 2016, Published online: 23 Jun 2016
 

ABSTRACT

The flow control constitutes a challenging research topic with numerous applications in aeronautics, aerodynamics, fluid mechanics, civil engineering, and so on. Due to the use of iterative algorithms, it is costly in both CPU time and memory requirements. In this paper, an optimal control strategy with reduced-order model built with proper orthogonal decomposition approach is proposed. The methodology is developed to control an anisothermal flow in a lid-driven cavity with one control parameter and then extended to at two control parameters. The control is realized in quasi-real time, which opens the way to promising practical applications.

Notes

1The parameters can be Reynolds number, Richardson number, Grashof number, …

2ω1 and ω2 are penalty terms of the objective functional to regularize the optimization problem [Citation47].

3The target temporal coefficient is associated to the target temperature field as:

(16)

It is obtained with the target control parameter αtar.

4The detail of the calculations is not given here. The reader can refer to the works of Joslin et al. [Citation48], in which the same methodology is employed on the momentum and mass conservation equations.

5The RIC is defined such as:

Table 1. Reconstruction POD error as a function of the POD mode number.

(29)
where λ are the eigenvalues, NPOD are the number of POD modes and Nsnap the number of snapshots.

6For this, new simulations with Code_Saturne have been realized.

7The classical method is a classical POD–ROM; the mean velocity field is decomposed according to the control function method ([Citation33, Citation34, Citation36, Citation37]):

(32)

us(x) corresponds to the solutions at large time of Navier–Stokes equations, i.e., the velocity snapshot with which the POD basis has been built and at the final time. Since , α and us(x) are known, it is straightforward to compute defined as .

8For this, news simulations with Code_Saturne have been realized.

9They must therefore be updated at each algorithm iteration.

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