使用M截断的分数导数在水力学非线性复杂方程中的一些新光学脉冲
Esin Ilhan1, Shafqat Ur Rehman2, Muhammad Bilal3
1Faculty of Engineering and Architecture, Kirsehir Ahi Evran University, Kirsehir, Turkey.
Scientific reports
|September 1, 2025
概括
研究人员使用分析方法探索了复杂的金兹堡-兰多方程波动. 新的单子解决方案被推导出,揭示了物理海洋学和非线性方程研究的各种波浪行为.
科学领域:
- 非线性动力学
- 数学物理
- 物理海洋学
背景情况:
- 复杂的Ginzburg-Landau (CGL) 方程模拟了各种物理系统中的波传播.
- 对于这些系统来说,了解单子溶液和动态波结构至关重要.
研究的目的:
- 在CGL方程中研究单子溶液和动态波结构.
- 通过先进的分析技术获得新的封闭式解决方案.
- 在分数导数的影响下探索这些解决方案的行为.
主要方法:
- 采用了库马尔-马利克方法,通用阿诺斯方法和能量平衡方法.
- 通过超标函数,三角函数和雅可比圆函数表达的精确解.
- 使用Mathematica进行验证,并生成图片进行可视化.
主要成果:
- 发现了精确的单独波的新家族和多样化的单独波解决方案.
- 观测到多波单体,复杂单体,单体和周期波.
- 可视化溶液行为,包括暗波和明波配置文件,与M截断的分数导数.
结论:
- 这项研究为物理海洋学中的波动提供了重要的见解.
- 获得的新解决方案为未来的非线性方程研究提供了基础.
- 这项工作增强了对复杂系统中孤独现象的理解.
更多相关视频
相关概念视频
Linear Approximation in Time Domain
124
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,...
124
Convergence of Fourier Series
201
The Fourier series is a powerful mathematical tool for representing periodic signals as an infinite sum of complex exponentials. In practice, this infinite series is truncated to a finite number of terms, yielding a partial sum. This truncation makes the approximation of the signal feasible but introduces certain challenges, particularly near discontinuities, known as the Gibbs phenomenon.
The Gibbs phenomenon refers to the persistent oscillations and overshoots that occur near discontinuities...
The Gibbs phenomenon refers to the persistent oscillations and overshoots that occur near discontinuities...
201
Second Derivatives and Laplace Operator
1.4K
The first order operators using the del operator include the gradient, divergence and curl. Certain combinations of first order operators on a scalar or vector function yield second order expressions. Second-order expressions play a very important role in mathematics and physics. Some second order expressions include the divergence and curl of a gradient function, the divergence and curl of a curl function, and the gradient of a divergence function.
Consider a scalar function. The curl of its...
Consider a scalar function. The curl of its...
1.4K
Damped Oscillations
6.0K
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...
6.0K
Transmission-Line Differential Equations
401
Transmission lines are essential components of electrical power systems. They are characterized by the distributed nature of resistance (R), inductance (L), and capacitance (C) per unit length. To analyze these lines, differential equations are employed to model the variations in voltage and current along the line.
Line Section Model
A circuit representing a line section of length Δx helps in understanding the transmission line parameters. The voltage V(x) and current i(x) are measured...
Line Section Model
A circuit representing a line section of length Δx helps in understanding the transmission line parameters. The voltage V(x) and current i(x) are measured...
401
Second Order systems II
169
In an underdamped second-order system, where the damping ratio ζ is between 0 and 1, a unit-step input results in a transfer function that, when transformed using the inverse Laplace method, reveals the output response. The output exhibits a damped sinusoidal oscillation, and the difference between the input and output is termed the error signal. This error signal also demonstrates damped oscillatory behavior. Eventually, as the system reaches a steady state, the error diminishes to zero.
169


