高云龙, 林荣瑞, 佘连兵, 李爱静. 带有强阻尼时滞项的m-Laplacian型波方程解的爆破[J]. 华南师范大学学报(自然科学版), 2021, 53(1): 94-99. doi: 10.6054/j.jscnun.2021015
引用本文: 高云龙, 林荣瑞, 佘连兵, 李爱静. 带有强阻尼时滞项的m-Laplacian型波方程解的爆破[J]. 华南师范大学学报(自然科学版), 2021, 53(1): 94-99. doi: 10.6054/j.jscnun.2021015
GAO Yunlong, LIN Rongrui, SHE Lianbing, LI Aijing. Blow-up of Solutions to the m-Laplacian Type Wave Equation with Strong Delay Terms[J]. Journal of South China Normal University (Natural Science Edition), 2021, 53(1): 94-99. doi: 10.6054/j.jscnun.2021015
Citation: GAO Yunlong, LIN Rongrui, SHE Lianbing, LI Aijing. Blow-up of Solutions to the m-Laplacian Type Wave Equation with Strong Delay Terms[J]. Journal of South China Normal University (Natural Science Edition), 2021, 53(1): 94-99. doi: 10.6054/j.jscnun.2021015

带有强阻尼时滞项的m-Laplacian型波方程解的爆破

Blow-up of Solutions to the m-Laplacian Type Wave Equation with Strong Delay Terms

  • 摘要: 研究带有强阻尼时滞项的m-Laplacian型波方程: u_tt-\Delta _mu-\Delta u+g*\Delta u-\mu _1\Delta u_t\left( x, t \right)-\mu _2\Delta u_t\left( x, t-\tau \right)=\left| u \right|^p-2u 解的爆破:当初始能量0 < E(0) < E1时, 利用能量函数构造凹函数L1(t), 得到微分不等式\frac\textdL_1\left( t \right)\textdt\ge \xi _0L_1^1+\nu \left( t \right)\ \left( \xi _0>0, \nu >0, t\ge 0 \right), 在(0, t)上对此微分不等式积分, 从而可知存在有限时间T*>0, 使得当时间t趋于T*时, 该m-Laplacian型波方程的解爆破; 当初始能量E(0) < 0时, 构造凹函数L2(t), 通过同样的方法得到该方程的解存在有限时间爆破.

     

    Abstract: Blow-up of solutions to the m-Laplacian type wave equation with strong delay was studied: u_tt-\Delta _mu-\Delta u+g*\Delta u-\mu _1\Delta u_t\left( x, t \right)-\mu _2\Delta u_t\left( x, t-\tau \right)=\left| u \right|^p-2u. When the initial energy 0 < E(0) < E1, the concave function L1(t) was constructed with the energy function, and the differential inequality \frac\textdL_1\left( t \right)\textdt\ge \xi _0L_1^1+\nu \left( t \right)\ \left( \xi _0>0, \nu >0, t\ge 0 \right) was obtained. Then, the differential inequality was integrated in (0, t), and it was proved that there was a finite time T*>0, so that when the time t was tended to T*, the m-Laplacian type wave equation underwent blow-up of solutions. When the initial energy E(0) < 0, a concave function L2(t) was also constructed. With the same method, it was found that the solutions to the equation had a finite-time blow-up.

     

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