Abstract:In this paper a modification of the 3-dimensional Navier-Stokes system which defines some system of quasilinear equations in Fourier space is considered. Properties of the obtained system and its finite-dimensional approximations are studied.
“…Property (1) is obvious, properties (2) and (3) are proven in [1]. To prove property (4), we note that det…”
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confidence: 93%
“…Here x = (x 1 , x 2 , x 3 ) ∈ R 3 , k = (k 1 , k 2 , k 3 ) ∈ R 3 andũ is pure imaginary and odd. Puttingũ(k, t) = iv(k, t) with v(−k, t) = −v(−k, t) we can write our approximation as a system of quasi-linear equations (see [1]):…”
mentioning
confidence: 99%
“…In what follows we consider systems (1) and (2) for ν ≥ 0 satisfying, at t = 0, the incompressibility condition (2). As was shown in [1], any solution v(k, t) satisfies the incompressibility condition (2) for all t for which a solution exists.…”
In this paper we consider a quasi-linear approximation for the 3D Euler system as well as for the Navier–Stokes system in our previous paper Moscow Math. J. 1(3) (2001), 381–388). We define finite-dimensional versions of the approximation and study properties of their solutions.
“…Property (1) is obvious, properties (2) and (3) are proven in [1]. To prove property (4), we note that det…”
mentioning
confidence: 93%
“…Here x = (x 1 , x 2 , x 3 ) ∈ R 3 , k = (k 1 , k 2 , k 3 ) ∈ R 3 andũ is pure imaginary and odd. Puttingũ(k, t) = iv(k, t) with v(−k, t) = −v(−k, t) we can write our approximation as a system of quasi-linear equations (see [1]):…”
mentioning
confidence: 99%
“…In what follows we consider systems (1) and (2) for ν ≥ 0 satisfying, at t = 0, the incompressibility condition (2). As was shown in [1], any solution v(k, t) satisfies the incompressibility condition (2) for all t for which a solution exists.…”
In this paper we consider a quasi-linear approximation for the 3D Euler system as well as for the Navier–Stokes system in our previous paper Moscow Math. J. 1(3) (2001), 381–388). We define finite-dimensional versions of the approximation and study properties of their solutions.
Properties of an infinite system of nonlinearly coupled ordinary differential equations are discussed. This system models some properties present in the equations of motion for an inviscid fluid such as the skew symmetry and the 3-dimensional scaling of the quadratic nonlinearity. In a companion paper [6] it is proved that every solution for the system with forcing blows up in finite time in the Sobolev H 5/6 norm. In this present paper, it is proved that after the blow-up time all solutions stay in H s , s < 5/6 for almost all time and the energy dissipates.Moreover, it is proved that the unique equilibrium is an exponential global attractor.
“…Recently, a number of simpler models have been proposed and studied by several authors as a way to gain insight into the possible behavior of solutions to Euler and Navier-Stokes equations. Different models have been suggested by Katz and Pavlović [9], Friedlander and Pavlović [5], Dinaburg and Sinaǐ [3], and Waleffe [13]. Although these models are fairly drastic simplifications of the original problem, they do keep a few of the most important characteristic features of the Euler equation.…”
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