在非线性粘弹性介质中通过卡普托-法布里齐奥分数运算符对膜振荡过程进行数学建模
Andriy Chaban1, Marek Lis2, Andriy Lozynskyy1
1Faculty of Transport, Electrical Engineering, and Computer Science, Casimir Pulaski Radom University, 26-600, Radom, Poland.
Scientific reports
|April 25, 2025
概括
本研究使用三种数学方法模拟粘弹性介质中的钢膜振荡. 纳入卡普托-法布里齐奥运营商增强了一个简化的模型.
科学领域:
- 机械工程 机械工程
- 应用数学 应用数学 应用数学
- 材料科学 材料科学 材料科学
背景情况:
- 钢膜在非线性粘弹性介质中振荡时表现出复杂的短暂行为.
- 准确的数学建模对于理解和预测这些动态过程至关重要.
研究的目的:
- 开发和比较三种不同的数学模型,用于振荡钢膜中的短暂过程.
- 评估不同的建模方法的有效性,包括微积分计算,以提高准确性.
主要方法:
- 使用修改的汉密尔顿-奥斯特罗格拉德斯基原理 (混合问题) 开发分布式参数模型.
- 将一个集中参数模型作为考西问题进行表述.
- 用卡普托-法布里齐奥演算子将分数导数和积分理论应用于简化的模型.
主要成果:
- 对所有三种模型类型进行了计算机模拟.
- 一项比较分析表明,卡普托-法布里齐奥运营商提高了简化膜模型的充分性.
- 分数计算方法提供了一个更准确的系统动态的表示.
结论:
- 卡普托-法布里齐奥操作器为提高粘弹性膜模型的准确性提供了一个有价值的工具.
- 分数计算为复杂机械系统的更精确的数学建模提供了一个有希望的途径.
- 该研究为根据所需的准确性和复杂性选择合适的模型提供了一个框架.
相关概念视频
Damped Oscillations
5.6K
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...
5.6K
Navier–Stokes Equations
201
For incompressible Newtonian fluids, where density remains constant, stresses show a linear relationship with the deformation rate, defined by normal and shear stresses. Normal stresses depend on the pressure exerted on the fluid and the rate of deformation in specific directions, which determines how fluid flows under varying pressures. Shear stresses, on the other hand, act tangentially across fluid layers. They explain how adjacent fluid layers slide relative to one another, connecting...
201
Types of Damping
6.3K
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...
6.3K
Oscillations about an Equilibrium Position
5.2K
Stability is an important concept in oscillation. If an equilibrium point is stable, a slight disturbance of an object that is initially at the stable equilibrium point will cause the object to oscillate around that point. For an unstable equilibrium point, if the object is disturbed slightly, it will not return to the equilibrium point. There are three conditions for equilibrium points—stable, unstable, and half-stable. A half-stable equilibrium point is also unstable, but is named so...
5.2K
Equations of Wave Motion
4.8K
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.
4.8K
Linear Approximation in Time Domain
56
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,...
56


