Abstract:We study the long-time behavior of the solution of a damped BBM equation ut + ux − uxxt + uux + Lγ (u) = 0. The proposed dampings Lγ generalize standards ones, as parabolic (Lγ (u) = −∆u) or weak damping (Lγ (u) = γu) and allows us to consider a greater range. After establish the local well-posedness in the energy space, we investigate some numerical properties.
“…We find in the literature different choices for L, depending on the physical situations, see [8,13,14,15,16,20,21,22,23,36,37] and [29] for physical experiments.…”
Section: Application To the Korteweg-de Vries Equationmentioning
We propose a simple numerical procedure to approach the symbol of a self-adjoint linear operator A by using trace estimates with numerical data. The Symbol Approximation Method (SAM) is based on an adaptation of the matrix trace estimator to successive distinct numerical spectral bands in order to build a piece-wise constant function as an approximation of the symbol σ of A. The decomposition of the spectral interval into band of frequencies is proposed with several approaches, from the formal spectral to the multi-grid one. We apply the new method to different operators when discretized in finite differences or in finite elements. The SAM is also proposed as a tool for the modeling of waves equations, and is presented a means to capture an additional linear damping term in hydrodynamics models such as Korteweig-de Vries or Benjamin Ono equations.
“…We find in the literature different choices for L, depending on the physical situations, see [8,13,14,15,16,20,21,22,23,36,37] and [29] for physical experiments.…”
Section: Application To the Korteweg-de Vries Equationmentioning
We propose a simple numerical procedure to approach the symbol of a self-adjoint linear operator A by using trace estimates with numerical data. The Symbol Approximation Method (SAM) is based on an adaptation of the matrix trace estimator to successive distinct numerical spectral bands in order to build a piece-wise constant function as an approximation of the symbol σ of A. The decomposition of the spectral interval into band of frequencies is proposed with several approaches, from the formal spectral to the multi-grid one. We apply the new method to different operators when discretized in finite differences or in finite elements. The SAM is also proposed as a tool for the modeling of waves equations, and is presented a means to capture an additional linear damping term in hydrodynamics models such as Korteweig-de Vries or Benjamin Ono equations.
“…At this point, we use ( 40) and obtain Unfortunately, in practice, this fixed point method converges only for very small values of ∆t. To enhance the stability region, and then to allow to take larger values of ∆t, we use the ∆ κ acceleration procedure introduced in [11] and applied in [1,2,19] for Allen-Cahn's, weakly damped Schrödinger and BBM equations respectively. In two words, the ∆ κ procedure consists in replacing the Picard iterates by…”
We present here different situations in which the filtering of high or low modes is used either for stabilizing semi-implicit numerical schemes when solving nonlinear parabolic equations, or for building adapted damping operators in the case of dispersive equation. We consider numerical filtering provided by mutigrid-like techniques as well as the filtering resulting from operator with monotone symbols. Our approach applies to several discretization techniques and we focus on finite elements and finite differences. Numerical illustrations are given on Cahn-Hilliard, Korteweig-de Vries and Kuramoto-Sivashinsky equations.
“…The proof will be done by using a fixed point argument. Therefore, the application of the following lemma, proved in [4], will be needed: and A is the compact operator defined by (10). Thus, we obtain that the solution of (74) is given by…”
Section: Remarkmentioning
confidence: 99%
“…Despite of the developments obtained for Boussinesq systems, there are many issues still open that deserves further attention, specially when dissipative mechanisms are incorporated to the models. In real physical situations, dissipative effects are often as important as nonlinear and dispersive effects (see, for instance, [5,6,10]) and this fact has given currency to the study of water wave model in nonlinear dispersive media. Indeed, it was clear from the experimental outcomes that damping effects must be accounted in addition to those of nonlinearity and dispersion for good quantitative agreement with model predictions.…”
In this paper we are concerned with a Boussinesq system for smallamplitude long waves arising in nonlinear dispersive media. Considerations will be given for the global well-posedness and the time decay rates of solutions when the model is posed on a periodic domain and a general class of damping operator acts in each equation. By means of spectral analysis and Fourier expansion, we prove that the solutions of the linearized system decay uniformly or not to zero, depending on the parameters of the damping operators. In the uniform decay case, the result is extended for the full system.
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