由有限时间波激发引起的共振逃逸
Pavel Kravetc1, Oleg Gendelman1, Alexander Fidlin2
1Faculty of Mechanical Engineering, Technion-Israel Institute of Technology, Haifa 3200003, Israel.
Chaos (Woodbury, N.Y.)
|June 5, 2023
概括
研究人员确定了振逃逸的临界强迫与减噪,并使用隔离振近似 (AIR) 方法来分析有限时间逃逸动态. 发现了一个类似碎形的边界,突出了AIR方法的局限性.
科学领域:
- * * 物理学 物理
- * 动态系统 动态系统
- * 混沌理论 *
背景情况:
- * 了解共振现象在各种物理和工程领域至关重要.
- * 湿系统中的有限时间逃生动态带来了复杂的挑战.
- * 隔离共振近似 (AIR) 是分析这些系统的常用方法.
研究的目的:
- * 为了确定在阻尼下在有限时间内响应逃逸所需的临界强迫.
- * 调整隔离共振近似 (AIR) 方法来分析有限时间逃逸.
- * 为了研究在相位和参数平面上逃逸时间的行为.
主要方法:
- *分析确定共振逃逸的临界强迫.
- * 隔离共振近似 (AIR) 方法的调整和应用.
- * 在相位和参数平面上对逃逸时间近似的数值分析.
主要成果:
- * 在有限的时间内获得了有阻尼的共振逃逸的临界强迫.
- * AIR方法已成功适应用于分析有限时间逃逸.
- * 确定了有限时间逃脱区域的新型碎形边界.
- *在相平面和参数平面上生成了逃逸时间近似值.
结论:
- *这项研究提供了关于化系统中共振逃逸的关键条件的见解.
- * 已识别的类似碎形的边界揭示了有限时间逃脱动态的复杂性.
- *这些发现增强了对隔离共振近似 (AIR) 方法局限性的理解.
- *结果解释了数值实验对这些系统整合时间的敏感性.
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