大学物理 ›› 2024, Vol. 43 ›› Issue (01): 37-.doi: 10.16854/j.cnki.1000-0712.220549

• 大学生园地 • 上一篇    下一篇

细棒入水动力学特性的解析计算与数值模拟

张宇锋,谢东,韦相忠,上官王佐   

  1. 1. 广西中医药大学 药学院及公管学院,广西 南宁530200;2. 贵州电子信息职业技术学院,贵州 凯里556000
  • 收稿日期:2022-11-06 修回日期:2023-03-02 出版日期:2024-03-01 发布日期:2024-03-06
  • 作者简介:张宇锋(2002—),男,广西南宁人,广西中医药大学公管学院2021级本科生.
  • 基金资助:
    广西中医药大学博士启动经费(2021BS008)资助

Analytical calculation and numerical simulation of  the dynamics of water-entry of a slender rod

ZHANG Yu-feng1, XIE Dong2, WEI Xiang-zhong1, SHANGGUAN Wang-zuo1   

  1. 1. College of Pharmacy and Public Management, Guangxi University of Chinese Medicine, Nanning, Guangxi 530200, China; 
    2. Guizhou Vocational Technology College of Electronic & Information, Kaili, Guizhou 556000, China
  • Received:2022-11-06 Revised:2023-03-02 Online:2024-03-01 Published:2024-03-06

摘要: 结合解析计算与数值模拟本文研究了均匀细棒低速入水过程中水的阻力系数和细棒密度这两个因素对其入水过程的动力学特性的影响.根据牛顿第二定律首先建立动力学微分方程并求得了解析解,由此进行数值计算并对其运动状态的动力学特性进行了分析.结果表明若细棒密度比水的大,不管以任何初速度入水,最终都会趋向于一个稳定的极限下沉速度,该极限速度正比于细棒与水的密度差,反比于水的阻力系数.但当密度差较小时,细棒的下沉速度先达到一个峰值,然后减速并逐渐趋向于稳定极限下沉速度.相反,如果细棒的密度不大于水的密度,则细棒入水后最终会静止不动而悬浮于水中.

关键词: 重物入水, 解析计算, 数值模拟, 极限下沉速度, 重物与水密度差

Abstract: Study on water-entry of heavy objects is of great importance to practical application and theoretical modeling, as it is widely present in daily life, and many fields of engineering and science as well. Combining theoretical derivation with numerical simulations, we study the impact of the damping coefficient of water and the density of the rod on the water-entry dynamics of a uniformly distributed rod at low velocity. The dynamic differential equation is established according to Newton's second law of motion and the analytical solution is obtained, based on which numerical simulations are carried out and the motion characteristics of the rod is analyzed. Numerical results show that a rod with greater density than that of water will eventually reach a stable maximum sinking speed, which is proportional to the density difference between the rod and the water, and inversely proportional to the damping coefficient of the water. The greater the density difference, the longer it takes to reach the maximum sinking speed. However, when the density difference is small, the velocity of the rod reaches a peak at first, and then it decelerates and gradually approaches the final sinking speed. The formation of velocity peak is reasonably accounted based on the forces acting on the rod and thus its acceleration variations. On the contrary, if the density of the rod is less than that of the water, it will eventually suspend in the water at still. Results also show that the smaller the damping coefficient of water, the longer it takes for the rod to reach the maximum sinking speed, and vice versa. The effect