AbstractWe consider the damped-driven KdV equation:u˙−νuxx+uxxx−6uux=νη(t,x),x∈S1,∫udx≡∫ηdx≡0, where 0<ν⩽1 and the random process η is smooth in x and white in t. For any periodic function u(x) let I=(I1,I2,…) be the vector, formed by the KdV integrals of motion, calculated for the potential u(x). We prove that if u(t,x) is a solution of the equation above, then for 0⩽t≲ν−1 and ν→0 the vector I(t)=(I1(u(t,⋅)),I2(u(t,⋅)),…) satisfies the (Whitham) averaged equation
AbstractConsider the stochastic Duffing–van der Pol equationẍ=−ω2x−Ax3−Bx2ẋ+ε2βẋ+εσxẆtwith A⩾0 a...
An averaging result is proved for stochastic evolution equations with highly oscillating coefficient...
Let there be giwQn a sequence of differential equations (1) X = =-À„X + S^{t, X, CD^), a sequence of...
International audienceWe consider the damped-driven KdV equation $$ \dot u-\nu{u_{xx}}+u_{xxx}-6uu_x...
We consider a perturbed KdV equation: [\dot{u}+u_{xxx} - 6uu_x = \epsilon f(x,u(\cdot)), \quad x\in ...
Abstract. For the damped-driven KdV equation u̇ − νuxx + uxxx − 6uux = ν η(t, x) , x ∈ S1, u dx ≡ η ...
International audienceFor the damped-driven KdV equation $$ \dot u-\nu{u_{xx}}+u_{xxx}-6uu_x=\sqrt\n...
International audienceWe consider KdV equation under periodic boundary conditions, perturbed by visc...
Averaging principle is an effective method for investigating dynamical systems with highly oscillati...
We study stochastic perturbations of linear systems of the form dv(t) + Av(t) dt = εP (v(t))dt + √ ε...
In this paper, we studied an averaging principle for Caputo–Hadamard fractional stochastic different...
In this note we give an overview of results concerning the Korteweg-deVries equation ut = −uxxx + 6u...
Consider the stochastic Duffing-van der Pol equation x ̈ = −ω2x − Ax3 −Bx2ẋ+ ε2βẋ+ εσxẆt with A ...
We analyze the classical problem of the stochastic dynamics of a particle confined in a periodic po...
Abstract: We study the evolution of the energy (mode-power) distribution for a class of randomly per...
AbstractConsider the stochastic Duffing–van der Pol equationẍ=−ω2x−Ax3−Bx2ẋ+ε2βẋ+εσxẆtwith A⩾0 a...
An averaging result is proved for stochastic evolution equations with highly oscillating coefficient...
Let there be giwQn a sequence of differential equations (1) X = =-À„X + S^{t, X, CD^), a sequence of...
International audienceWe consider the damped-driven KdV equation $$ \dot u-\nu{u_{xx}}+u_{xxx}-6uu_x...
We consider a perturbed KdV equation: [\dot{u}+u_{xxx} - 6uu_x = \epsilon f(x,u(\cdot)), \quad x\in ...
Abstract. For the damped-driven KdV equation u̇ − νuxx + uxxx − 6uux = ν η(t, x) , x ∈ S1, u dx ≡ η ...
International audienceFor the damped-driven KdV equation $$ \dot u-\nu{u_{xx}}+u_{xxx}-6uu_x=\sqrt\n...
International audienceWe consider KdV equation under periodic boundary conditions, perturbed by visc...
Averaging principle is an effective method for investigating dynamical systems with highly oscillati...
We study stochastic perturbations of linear systems of the form dv(t) + Av(t) dt = εP (v(t))dt + √ ε...
In this paper, we studied an averaging principle for Caputo–Hadamard fractional stochastic different...
In this note we give an overview of results concerning the Korteweg-deVries equation ut = −uxxx + 6u...
Consider the stochastic Duffing-van der Pol equation x ̈ = −ω2x − Ax3 −Bx2ẋ+ ε2βẋ+ εσxẆt with A ...
We analyze the classical problem of the stochastic dynamics of a particle confined in a periodic po...
Abstract: We study the evolution of the energy (mode-power) distribution for a class of randomly per...
AbstractConsider the stochastic Duffing–van der Pol equationẍ=−ω2x−Ax3−Bx2ẋ+ε2βẋ+εσxẆtwith A⩾0 a...
An averaging result is proved for stochastic evolution equations with highly oscillating coefficient...
Let there be giwQn a sequence of differential equations (1) X = =-À„X + S^{t, X, CD^), a sequence of...