2019
DOI: 10.1002/num.22382
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A linear, decoupled fractional time‐stepping method for the nonlinear fluid–fluid interaction

Abstract: In this paper, a linear decoupled fractional time stepping method is proposed and developed for the nonlinear fluid–fluid interaction governed by the two Navier–Stokes equations. Partitioned time stepping method is applied to two‐physics problems with stiffness of the coupling terms being treated explicitly and is also unconditionally stable. As for each fluid, the velocity and pressure are respectively determined by just solving one vector‐valued quasi‐elliptic equation and the Possion equation with homogeneo… Show more

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Cited by 17 publications
(6 citation statements)
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References 39 publications
(59 reference statements)
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“…Moreover, we achieve a series of numerical results for the presented problem [21][22][23]. Furthermore, we will then use the efficient methods [18,34,35,37] to solve the similar practical problem for the coupling problem.…”
Section: Resultsmentioning
confidence: 99%
“…Moreover, we achieve a series of numerical results for the presented problem [21][22][23]. Furthermore, we will then use the efficient methods [18,34,35,37] to solve the similar practical problem for the coupling problem.…”
Section: Resultsmentioning
confidence: 99%
“…Theorem 2 (Unconditional stability of MBELF scheme) Let u n+1 ∈ X h satisfy (12) for n = 1, 2, … , N − 1, there exist a constant C independent of Δt and h, such that…”
Section: Stabilities Of Numerical Algorithmsmentioning
confidence: 99%
“…Besides, Qian et al studied a fully discrete Crank–Nicolson leap‐frog (CNLF) time stepping decoupled scheme for atmosphere–ocean coupling system [11], the nonlinear interface term still decoupled by using GA strategy for the interface jump term. In the meantime, Li et al proposed a linear decoupled fractional time stepping method [12], for each fluid, the velocity, and pressure were respectively determined by just solving one vector‐valued quasi‐elliptic equation and the Poisson equation with homogeneous Neumann boundary condition per time step. They also proposed a parallel non‐spatial iterative and rotational pressure projection method in Reference [13].…”
Section: Introductionmentioning
confidence: 99%
“…Then, the weak formulation of the dual-porosity-Navier-Stokes model (2.1)-(2.12) as follows [31][32][33][34][35][36]. we suppose ⃗ f s ∈ H −1 (Ω s ) and f d ∈ L 2 (Ω d ).…”
Section: Preliminaries Weak Formulations and Finite Element Spacesmentioning
confidence: 99%