Behavior of solutions to a Petrovsky equation with damping and variable-exponent sources
نویسندگان
چکیده
This paper deals with the following Petrovsky equation damping and nonlinear sources: $${u_{tt}} + {\Delta ^2}u - M\left({\left\| {\nabla u} \right\|_2^2} \right)\Delta u \Delta {u_t} {\left| {{u_t}} \right|^{m(x) 2}}{u_t} = \right|^{p(x) 2}}u$$ under initial-boundary value conditions, where M(s) a bsγ is positive C1 function parameters > 0, b γ ⩾ 1, m(x) p(x) are given measurable functions. The upper bound of blow-up time derived for low initial energy by differential inequality technique. For ≡ 2, in particular, obtained combination Levine’s concavity method some inequalities high energy. In addition, we discuss lower making full use strong damping. Moreover, present global existence solutions an decay estimate establishing estimates.
منابع مشابه
a comparison of teachers and supervisors, with respect to teacher efficacy and reflection
supervisors play an undeniable role in training teachers, before starting their professional experience by preparing them, at the initial years of their teaching by checking their work within the proper framework, and later on during their teaching by assessing their progress. but surprisingly, exploring their attributes, professional demands, and qualifications has remained a neglected theme i...
15 صفحه اولBEHAVIOR OF SOLUTIONS TO A FUZZY NONLINEAR DIFFERENCE EQUATION
In this paper, we study the existence, asymptotic behavior of the positive solutions of a fuzzy nonlinear difference equation$$ x_{n+1}=frac{Ax_n+x_{n-1}}{B+x_{n-1}}, n=0,1,cdots,$$ where $(x_n)$ is a sequence of positive fuzzy number, $A, B$ are positive fuzzy numbers and the initial conditions $x_{-1}, x_0$ are positive fuzzy numbers.
متن کاملCritical Exponent for a Nonlinear Wave Equation with Damping
It is well known that if the damping is missing, the critical exponent for the nonlinear wave equation gu=|u| p is the positive root p0(n) of the equation (n&1) p&(n+1) p&2=0, where n 2 is the space dimension (for p0(1)= , see Sideris [14]). The proof of this fact, known as Strauss' conjecture [17], took more than 20 years of effort, beginning with Glassey doi:10.1006 jdeq.2000.3933, available ...
متن کاملBlow-Up of Solutions for a System of Petrovsky Equations with an Indirect Linear Damping
In this paper, we consider a coupled system of Petrovsky equations in a bounded domain with clamped boundary conditions. Due to several physical considerations, a linear damping which is distributed everywhere in the domain under consideration appears only in the first equation whereas no damping term is applied to the second one (this is indirect damping). Many studies show that the solution o...
متن کاملExistence of Solutions to a Nonlinear Parabolic Equation of Fourth-Order in Variable Exponent Spaces
Abstract: This paper is devoted to studying the existence and uniqueness of weak solutions for an initial boundary problem of a nonlinear fourth-order parabolic equation with variable exponent vt + div(|∇4v|p(x)−2∇4v) − |4v|q(x)−24v = g(x, v). By applying Leray-Schauder’s fixed point theorem, the existence of weak solutions of the elliptic problem is given. Furthermore, the semi-discrete method...
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
ژورنال
عنوان ژورنال: Science China-mathematics
سال: 2022
ISSN: ['1674-7283', '1869-1862']
DOI: https://doi.org/10.1007/s11425-021-1926-x