华南理工大学学报(自然科学版) ›› 2009, Vol. 37 ›› Issue (6): 117-123.

• 力学 • 上一篇    下一篇

畸形波生成的一种非线性机理分析

张运秋1  胡金鹏2   

  1. 1. 中国科学院 可再生能源与天然气水合物重点实验室, 广东 广州 510640; 2. 华南理工大学 土木与交通学院, 广东 广州 510640
  • 收稿日期:2008-09-08 修回日期:2008-11-18 出版日期:2009-06-25 发布日期:2009-06-25
  • 通信作者: 张运秋(1974-),女,助理研究员,博士,主要从事非线性波浪模拟及波浪能转换研究. E-mail:zhangyq6@ms.giec
  • 作者简介:张运秋(1974-),女,助理研究员,博士,主要从事非线性波浪模拟及波浪能转换研究.
  • 基金资助:

    国家“863”计划项目(2006AA052426,2006AA05Z251)

Analysis of a Nonlinear Generation Mechanism of Freak Waves

Zhang Yun-qiu1  Hu Jin-peng2   

  1. 1. Key Laboratory of Renewable Energy and Gas Hydrate, Chinese Academy of Sciences, Guangzhou 510640, Guangdong, China; 2. School of Civil Engineering and Transportation, South China University of Technology, Guangzhou 510640, Guangdong, China
  • Received:2008-09-08 Revised:2008-11-18 Online:2009-06-25 Published:2009-06-25
  • Contact: 张运秋(1974-),女,助理研究员,博士,主要从事非线性波浪模拟及波浪能转换研究. E-mail:zhangyq6@ms.giec
  • About author:张运秋(1974-),女,助理研究员,博士,主要从事非线性波浪模拟及波浪能转换研究.
  • Supported by:

    国家“863”计划项目(2006AA052426,2006AA05Z251)

摘要: 根据畸形波的非线性特点,采用控制深水波列演化的四阶修正非线性薛定谔方程,基于缓慢调制波列演化的边带不稳定性,研究了边带扰动条件下畸形波的生成与复波包谱的变化,并进一步分析了满足边带不稳定条件时,扰动频带宽度、初始扰动振幅、波陡及非线性阶数对边带不稳定性的发展和畸形波生成的影响.结果表明:载波能量向与之频率较近的不稳定边带的快速转移,可使波列在局部迅速增长而生成畸形波,因此该能量转移特性是边带不稳定性导致畸形波生成的一个根本原因;另外,较窄的扰动频带宽度、较大的扰动振幅、较大的波陡和较强的非线性均有利于边带不稳定性的发展和畸形波的生成.

关键词: 畸形波, 非线性薛定谔方程, 边带不稳定性, 非线性机理

Abstract:

According to the nonlinearity of freak waves and the sideband instability existing in the evolution of slowly-modulated periodic wave trains, the modified four-order nonlinear Schrodinger equation is employed to investigate the generation of freak waves and the variation of the corresponding complex wave-envelope spectra in the condition of sideband disturbances. Then, with the sideband instability being satisfied, the influences of the disturbance fre- quency bandwidth, the initial disturbance amplitude, the wave steepness and the nonlinear order on the develop- ment of sideband instability and on the occurrence of freak waves are analyzed. The results show that the occurrence of freak waves is due to the local exponential growth of the wave train because the carrier wave energy rapidly transfers to the neighbourly-unstable sideband components. Thus, energy transfer is a main reason for the occurrence of freak waves in the condition of sideband disturbances. It is also indicated that narrow frequency bandwidth, high disturbance amplitude, large wave steepness and strong nonlinearity all contribute favorably to the development of sideband instability and to the occurrence of freak waves.

Key words: freak wave, nonlinear Schrodinger equation, sideband instability, nonlinear mechanism