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Infinite superlinear growth of the gradient for the two-dimensional Euler equation

Infinite superlinear growth of the gradient for the two-dimensional Euler equation DISCRETE AND CONTINUOUS Website: http://aimSciences.org DYNAMICAL SYSTEMS Volume 23, Number 3, March 2009 pp. 1–XX INFINITE SUPERLINEAR GROWTH OF THE GRADIENT FOR THE TWO-DIMENSIONAL EULER EQUATION Sergey A. Denisov University of Wisconsin-Madison, Mathematics Department 480 Lincoln Dr. Madison, WI 53706-1388, USA (Communicated by Roger Temam) Abstract. For two-dimensional Euler equation on the torus, we prove that the L norm of the gradient can grow superlinearly for some infinitely smooth initial data. We also show the exponential growth of the gradient for finite time. 1. Introduction. In this note, we are dealing with two-dimensional Euler equation. We will write the equation for vorticity in the following form ⊥ −1 θ = ∇θ · u, u = ∇ ζ = (ζ ,−ζ ), ζ = Δ θ, θ(x, y, 0) = θ (x, y) y x 0 and θ is 2π–periodic in both x and y (e.g., the equation is considered on the torus −1 T). We assume that θ has zero average over T and then Δ is well-defined since the Euler flow is area-preserving and the average of θ(·, t) is zero as well. The global existence of the smooth solution for smooth initial data is well-known [2]. It http://www.deepdyve.com/assets/images/DeepDyve-Logo-lg.png Discrete and Continuous Dynamical Systems Unpaywall

Infinite superlinear growth of the gradient for the two-dimensional Euler equation

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Publisher
Unpaywall
ISSN
1078-0947
DOI
10.3934/dcds.2009.23.755
Publisher site
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Abstract

DISCRETE AND CONTINUOUS Website: http://aimSciences.org DYNAMICAL SYSTEMS Volume 23, Number 3, March 2009 pp. 1–XX INFINITE SUPERLINEAR GROWTH OF THE GRADIENT FOR THE TWO-DIMENSIONAL EULER EQUATION Sergey A. Denisov University of Wisconsin-Madison, Mathematics Department 480 Lincoln Dr. Madison, WI 53706-1388, USA (Communicated by Roger Temam) Abstract. For two-dimensional Euler equation on the torus, we prove that the L norm of the gradient can grow superlinearly for some infinitely smooth initial data. We also show the exponential growth of the gradient for finite time. 1. Introduction. In this note, we are dealing with two-dimensional Euler equation. We will write the equation for vorticity in the following form ⊥ −1 θ = ∇θ · u, u = ∇ ζ = (ζ ,−ζ ), ζ = Δ θ, θ(x, y, 0) = θ (x, y) y x 0 and θ is 2π–periodic in both x and y (e.g., the equation is considered on the torus −1 T). We assume that θ has zero average over T and then Δ is well-defined since the Euler flow is area-preserving and the average of θ(·, t) is zero as well. The global existence of the smooth solution for smooth initial data is well-known [2]. It

Journal

Discrete and Continuous Dynamical SystemsUnpaywall

Published: Nov 18, 2008

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