在分数导数设置中的水力动力学非线性复杂模型中单一波的传播
Muhammad Bilal1, Yazen M Alawaideh2, Shafqat Ur Rehman3
1Department of Physics, Shanghai University, Shanghai, 200444, China.
Scientific reports
|December 1, 2025
概括
这项研究使用新的分析方法探索了复杂的金兹堡-兰多方程动态,揭示了各种单元解和波浪行为. 新的精确单一波解决方案得出并可视化,推进非线性波研究.
科学领域:
- 非线性动力学是一种非线性动力学.
- 数学物理学的数学物理.
背景情况:
- 复杂的金兹堡-兰道方程模拟了超导,非线性光学和液晶中的现象.
- 了解它的单子解和波动力学对于各种科学领域至关重要.
研究的目的:
- 为了研究复杂的金兹堡-兰多方程的单子解和动态波动行为.
- 应用新的分析技术来获得精确的封闭式溶液.
主要方法:
- 采用了新的理性扩展的辛特-戈登方程扩展方法 (ShGEEM).
- 使用了修改的泛指数理函数方法 (mGERFM).
- 使用Mathematica验证的解决方案和可视化动态与2D/3D图片的分数顺序导数.
主要成果:
- 通过使用ShGEEM获得了精确的单一波解的新家族.
- 使用mGERFM.FM获得过度,三角形和指数解.
- 确定了各种单独的结构,包括复杂的,单一的,明亮的,黑暗的和多波形状.
结论:
- 该研究成功地利用ShGEEM和mGERFM获得了复杂的Ginzburg-Landau方程的新确切解决方案.
- 这些发现增强了对非线性波动力学的理解,特别是在分数顺序模型中.
- 这项研究开创了ShGEEM和mGERFM对这个特定方程的应用.
更多相关视频
相关概念视频
Propagation of Waves
2.8K
When a wave propagates from one medium to another, part of it may get reflected in the first medium, and part of it may get transmitted to the second medium. In such a case, the interface of the two mediums can be considered as a boundary that is neither fixed nor free.
Consider a scenario where a wave propagates from a string of low linear mass density to a string of high linear mass density. In such a case, the reflected wave is out of phase with respect to the incident wave, however the...
Consider a scenario where a wave propagates from a string of low linear mass density to a string of high linear mass density. In such a case, the reflected wave is out of phase with respect to the incident wave, however the...
2.8K
Linear Approximation in Time Domain
310
Nonlinear systems often require sophisticated approaches for accurate modeling and analysis, with state-space representation being particularly effective. This method is especially useful for systems where variables and parameters vary with time or operating conditions, such as in a simple pendulum or a translational mechanical system with nonlinear springs.
For a simple pendulum with a mass evenly distributed along its length and the center of mass located at half the pendulum's length,...
For a simple pendulum with a mass evenly distributed along its length and the center of mass located at half the pendulum's length,...
310
Damped Oscillations
6.7K
In the real world, oscillations seldom follow true simple harmonic motion. A system that continues its motion indefinitely without losing its amplitude is termed undamped. However, friction of some sort usually dampens the motion, so it fades away or needs more force to continue. For example, a guitar string stops oscillating a few seconds after being plucked. Similarly, one must continually push a swing to keep a child swinging on a playground.
Although friction and other non-conservative...
Although friction and other non-conservative...
6.7K
Types of Damping
7.5K
If the amount of damping in a system is gradually increased, the period and frequency start to become affected because damping opposes, and hence slows, the back and forth motion (the net force is smaller in both directions). If there is a very large amount of damping, the system does not even oscillate; instead, it slowly moves toward equilibrium. In brief, an overdamped system moves slowly towards equilibrium, whereas an underdamped system moves quickly to equilibrium but will oscillate about...
7.5K
Wave Parameters
8.9K
The simplest mechanical waves are associated with simple harmonic motion and repeat themselves for several cycles. These simple harmonic waves can be modeled using a combination of sine and cosine functions. Consider a simplified surface water wave that moves across the water's surface. Unlike complex ocean waves, in surface water waves, water moves vertically, oscillating up and down, whereas the disturbance of the wave moves horizontally through the medium. If a seagull is floating on the...
8.9K
Equations of Wave Motion
8.2K
Mathematically, the motion of a wave can be studied using a wavefunction. Consider a string oscillating up and down in simple harmonic motion, having a period T. The wave on the string is sinusoidal and is translated in the positive x-direction as time progresses. Sine is a function of the angle θ, oscillating between +A and −A and repeating every 2π radians. To construct a wave model, the ratio of the angle θ and the position x is considered.
8.2K


