2020
DOI: 10.3934/eect.2020031
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Approximate continuous data assimilation of the 2D Navier-Stokes equations via the Voigt-regularization with observable data

Abstract: We propose a data assimilation algorithm for the 2D Navier-Stokes equations, based on the Azouani, Olson, and Titi (AOT) algorithm, but applied to the 2D Navier-Stokes-Voigt equations. Adapting the AOT algorithm to regularized versions of Navier-Stokes has been done before, but the innovation of this work is to drive the assimilation equation with observational data, rather than data from a regularized system. We first prove that this new system is globally well-posed. Moreover, we prove that for any admissibl… Show more

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Cited by 18 publications
(6 citation statements)
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“…Dissipation is then crucially used to prove that the system converges not only to the observed projection of the true state, but in fact to the full true state. It was noted in [16,33,54] for different systems that if the parameters of the model are not that of the true state, then the system will converge to a finite amount of unrecoverable error. This remaining error is a direct consequence of the parameter error, and hence provides an avenue to estimating the true value of the parameter.…”
Section: Introductionmentioning
confidence: 99%
“…Dissipation is then crucially used to prove that the system converges not only to the observed projection of the true state, but in fact to the full true state. It was noted in [16,33,54] for different systems that if the parameters of the model are not that of the true state, then the system will converge to a finite amount of unrecoverable error. This remaining error is a direct consequence of the parameter error, and hence provides an avenue to estimating the true value of the parameter.…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, inspired by the methodology of data assimilation, especially variational data assimilation in continuous time (for relevant works we refer e.g. to [13,19,26,29,30,44,46,52]), we seek to minimise the misfit functional (u, p, y) → (1 − λ) Q(•, •, u, ∇u, p) − q + λ y over all admissible triplets (u, p, y) which satisfy (1.1), for a fixed weight λ ∈ (0, 1). The role of this weight is to obtain essentially a Pareto family of extremals, one for each value λ, even though in this paper we do not pursue further this viewpoint of vector-valued minimisation (the interested reader may e.g.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…In such methods, nudging of the computed solution is done by penalizing its difference to measurement data, that is, I H ( v ) is penalized to be close to I H ( u ). Since the initial work of Azouani et al in 2014 [4], there has been a large amount of work done for these types of methods, including for many different equations arising from physics such as Navier–Stokes equations (NSE) and Boussinesq, for different variations of DA implementation, and noisy data: CDA for NSE is studied in [7, 18, 42], with noisy data [6], noisy data discrete in time [20], and fully discrete [37]; CDA for NS‐ α is considered in [1] for higher Reynolds number flow; CDA is applied to Benard convection in [2, 16, 19] with various methods of nudging; CDA for Brinkman Forchheimer‐extended Darcy is studied in [43] and for surface quasi‐geostrophic equation in [34]; general interpolating operators for CDA are considered in [21]; CDA for reduced order modeling of the NSE is studied in [50]; and nonlinear nudging is proposed and analyzed in [36]. Although most of these works are in 2D, some research has been done in 3D including good numerical results for CDA applied to the 3D NSE in [40, 41] and analytical results for 3D Leray‐ α [17] and NS‐ α [1].…”
Section: Introductionmentioning
confidence: 99%