Asymptotic Stability for a Class of the Third-Grade Fluids Equations
The third-grade fluid equations are a type of Navier–Stokes equation with perturbations, where the perturbation term is given by a third-grade fluid. This article primarily investigates the large-time behavior for a class of third-grade fluid equations ...
Juan Song, Tianli Li
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Mécaniques des fluides et mécaniques quantiques Fluid Mechanics and Quantum Mechanics
Cette étude présente une méthode pour transformer les équations de Navier Stokes en l'équation de Schrddinger. Cette transformation permet le calcul simple des efforts de trainée et de portance sur un cylindre de longueur infinie en écoulement uniforme ...
Scmitt J.
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Mixed Finite Element Formulation for Navier-Stokes Equations for Magnetic Effects on Biomagnetic Fluid in a Rectangular Channel. [PDF]
Kasiman EH +7 more
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Stochastic Navier-Stokes Equations on a Thin Spherical Domain. [PDF]
Brzeźniak Z, Dhariwal G, Le Gia QT.
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Active training of physics-informed neural networks to aggregate and interpolate parametric solutions to the Navier-Stokes equations. [PDF]
Arthurs CJ, King AP.
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Invariant Measures for the Stochastic One-Dimensional Compressible Navier-Stokes Equations. [PDF]
Coti Zelati M, Glatt-Holtz N, Trivisa K.
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This article is devoted to the study of the nonhomogeneous incompressible Navier-Stokes equations in space dimension three. By making use of the "weakly nonlinear" energy estimate approach introduced by Lei and Zhou in [16], we establish two ...
Qianqian Hou, Xiaojing Xu, Zhuan Ye
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The nested block preconditioning technique for the incompressible Navier-Stokes equations with emphasis on hemodynamic simulations. [PDF]
Liu J, Yang W, Dong M, Marsden AL.
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COMPUTING ILL-POSED TIME-REVERSED 2D NAVIER-STOKES EQUATIONS, USING A STABILIZED EXPLICIT FINITE DIFFERENCE SCHEME MARCHING BACKWARD IN TIME. [PDF]
Carasso AS.
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Partial Regularity for Navier-Stokes Equations
We prove, with a more geometric approach, that the solutions to the Navier-Stokes equations are regular up to a set of Hausdorff dimension 1. The main tool for the proof is a new compactness lemma and the monotonicity property of harmonic functions.
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