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[PDF] Top 20 Blow up of Solutions for a System of Nonlinear Higher order Kirchhoff type Equations

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Blow up of Solutions for a System of Nonlinear Higher order Kirchhoff type Equations

Blow up of Solutions for a System of Nonlinear Higher order Kirchhoff type Equations

... a nonlinear damping ...the nonlinear case (p > 1). They showed that solutions with negative initial energy blow up in finite ...the nonlinear damping and the solution has ... See full document

11

Exponential energy decay and blow-up of solutions for a system of nonlinear viscoelastic wave equations with strong damping

Exponential energy decay and blow-up of solutions for a system of nonlinear viscoelastic wave equations with strong damping

... the equations, they established several results concerning local existence, glo- bal existence, uniqueness, and finite time blow-up (the initial energy E(0) < 0) ...latter blow-up ... See full document

19

Global Existence, Asymptotic Behavior and Blow-up of Solutions for a Suspension Bridge Equation with Nonlinear Damping and Source Terms

Global Existence, Asymptotic Behavior and Blow-up of Solutions for a Suspension Bridge Equation with Nonlinear Damping and Source Terms

... for blow-up ...for blow-up time of a system of ...for blow-up time of the solutions to two nonlinear wave ... See full document

25

Blow-up of solutions to a class of Kirchhoff equations with strong damping and nonlinear dissipation

Blow-up of solutions to a class of Kirchhoff equations with strong damping and nonlinear dissipation

... the system toward stability, while the nonlinear source term f (u) models an external force that amplifies the energy and drives the system to possible solutions that blow up in ... See full document

10

Long-Time Behavior of Solutions for a Class of Nonlinear Higher Order Kirchhoff Equation

Long-Time Behavior of Solutions for a Class of Nonlinear Higher Order Kirchhoff Equation

... [17] Ling Chen, Wei Wang, Guoguang Lin. The global attractor and their Hausdorff and Fractal dimensions estimation for the higher-order nonlinear Kirchhoff-type equation [J]. ... See full document

9

Existence of Random Attractor Family for a Class of Nonlinear Higher Order Kirchhoff Equations

Existence of Random Attractor Family for a Class of Nonlinear Higher Order Kirchhoff Equations

... u x = u x u x = u x (8) where u u x t = ( ) , is the real function on U × [ 0, +∞ ) , α > 0 is the strong damping coefficient, β > 0 is the damping coefficient, and K > 0 is the dis- sipation coefficient. In ... See full document

12

The Inertial Manifold for a Class of Nonlinear Higher Order Coupled Kirchhoff Equations with Strong Linear Damping

The Inertial Manifold for a Class of Nonlinear Higher Order Coupled Kirchhoff Equations with Strong Linear Damping

... for nonlinear Kirchhoff type equations with higher-order strong damping is considered by using the Hadamard graph transformation ...in order to acquire the result of the ... See full document

13

Random Attractor of the Stochastic Strongly Damped for the Higher Order Nonlinear Kirchhoff Type Equation

Random Attractor of the Stochastic Strongly Damped for the Higher Order Nonlinear Kirchhoff Type Equation

... This paper is organized as follows: In Section 2, we recall many basic concepts related to a random attractor for genneral random dynamical system. In Section 3, we introduce O-U process and deal with random term. ... See full document

11

Random Attractor Family for the Kirchhoff Equation of Higher Order with White Noise

Random Attractor Family for the Kirchhoff Equation of Higher Order with White Noise

... of solutions of sto- chastic higher-order Kirchhoff equation with strong damping of white noise, nonlinear and non-local source terms and the existence of attractors of stochas- tic ... See full document

11

7. On solutions of a system of higher-order nonlinear fractional differential equations

7. On solutions of a system of higher-order nonlinear fractional differential equations

... (the nonlinear alternative of Leray-Schauder) Let X be a normed linear space, S ⊂ X be a convex set, U be open in S with 0 ∈ U, and F : U → S be a continuous and compact ... See full document

10

The Inertial Manifolds for a Class of Higher Order Coupled Kirchhoff Type Equations

The Inertial Manifolds for a Class of Higher Order Coupled Kirchhoff Type Equations

... coupled Kirchhoff-type ...the system. For this problem, we will study the exponential attractors, blow-up, random attractors and so ... See full document

10

On Local Existence and Blow Up of Solutions for Nonlinear Wave Equations of Higher Order Kirchhoff Type with Strong Dissipation

On Local Existence and Blow Up of Solutions for Nonlinear Wave Equations of Higher Order Kirchhoff Type with Strong Dissipation

... and blow-up of solutions for nonlinear wave equations of higher-order Kirchhoff type with strong ...nondenerate Kirchhoff equation, and derive the ... See full document

15

Estimate on the Dimension of Global Attractor for Nonlinear Higher Order Coupled Kirchhoff Type Equations

Estimate on the Dimension of Global Attractor for Nonlinear Higher Order Coupled Kirchhoff Type Equations

... G. G. Lin and L. J., Hu have studied the existence of a global attractor for coupled Kirchhoff type equations with strongly linear damping in [1]. In this paper, we are concerned with the finite ... See full document

14

Finite time blow up of solutions of the Kirchhoff-type equation with variable exponents

Finite time blow up of solutions of the Kirchhoff-type equation with variable exponents

... Ikehata, On global solutions and energy decay for the wave equations of the Kirchhoff type with nonlinear damping terms, J.. Messaoudi, Blow up in a nonlinearly damped wave equation, Mat[r] ... See full document

9

The Global Attractors for the Higher Order Kirchhoff Type Equation with Nonlinear Strongly Damped Term

The Global Attractors for the Higher Order Kirchhoff Type Equation with Nonlinear Strongly Damped Term

... ∂ − ∂ ∆ − ∆ + = ∇ ⋅ ∇ + (1.6) In bounded 3D domains. This method establishes the existence and uniqueness of energy solutions in the case where the growth exponent of the non-linearity φ is less than 6 and f may ... See full document

16

Existence and concentration of solutions for the nonlinear Kirchhoff type equations with steep well potential

Existence and concentration of solutions for the nonlinear Kirchhoff type equations with steep well potential

... The paper is organized as follows. In Section , we introduce some notations and the variational framework for (.), and then establish compactness conditions. In Section , we prove Theorem . and Theorem .. In the ... See full document

15

On the decay and blow up of solutions for a quasilinear hyperbolic equations with nonlinear damping and source terms

On the decay and blow up of solutions for a quasilinear hyperbolic equations with nonlinear damping and source terms

... tion between the linear damping (q = ) and source term by using a concavity method. But this method cannot be applied in the case of a nonlinear damping term. Georgiev and Todorova [] extended Levine’s result to ... See full document

14

Blow up of the Solutions of Nonlinear Wave Equation

Blow up of the Solutions of Nonlinear Wave Equation

... Georgiev, “Blow up of the solutions of nonlinear wave equation in Reissner-Nordstr¨om metric,” Dynamics of Partial Di ff erential Equations , vol.[r] ... See full document

51

Nonoscillatory solutions for higher order nonlinear neutral delay differential equations

Nonoscillatory solutions for higher order nonlinear neutral delay differential equations

... 2 The existence of uncountably many bounded nonoscillatory solutions Now we investigate sufficient conditions for the existence of uncountably many bounded nonoscillatory solutions of (.) under various ... See full document

34

Blow up problems for a degenerate parabolic equation with nonlocal source and nonlocal nonlinear boundary condition

Blow up problems for a degenerate parabolic equation with nonlocal source and nonlocal nonlinear boundary condition

... where a, l > 0 and Ω is a bounded domain in R N (N ≥ 1) with smooth boundary ∂Ω . There have been many articles dealing with properties of solutions to degenerate parabolic equations with homogeneous ... See full document

14

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