对哈密尔顿式和波器的复杂时间方法
1Department of Mechanical Engineering, University of the Peloponnese, 26334 Patras, Greece.
Entropy (Basel, Switzerland)
|August 28, 2025
概括
定量几何热力学 (QGT) 统一了不可逆转的热力学,通过使用复杂时间来推导波器的哈密尔顿式. 这种方法提供了一个与简易几何相一致的新几何框架.
科学领域:
- 热力学
- 几何力学
- 非线性动力学
背景情况:
- 减压波器 (DHO) 是物理学中的一个基本模型,但在哈密尔顿力学中描述它,尤其是在所有减压模式中,都带来了挑战.
- 现有的不可逆热力学框架往往缺乏统一的几何方法.
研究的目的:
- 通过使用定量几何热力学 (QGT) 形式来推导适用于所有减压模式的减压波器 (DHO) 的哈密尔顿数.
- 为不可逆转的热力学建立统一的几何框架.
主要方法:
- 复杂时间的引入,其中真实和虚构部分分别代表产量和可逆动态.
- 应用定量几何热力学 (QGT) 形式来推导 DHO 哈密尔顿式.
- 与Caldirola-Kanai和GENERIC等现有框架进行比较.
主要成果:
- 通过QGT获得复杂生成的通用DHO哈密尔顿式,适用于所有缓解方案.
- 衍生的哈密尔顿式表现出一个修改的波桑括号结构,包含热力学不可逆转性.
- 来自QGT的哈密尔顿式与卡尔迪罗拉-卡奈哈密尔顿式相匹配,验证了QGT方法.
结论:
- 定量几何热力学 (QGT) 为不可逆转的热力学提供了一个优雅而一致的几何框架.
- QGT形式主义为扩展哈密尔顿力学到消散系统提供了一种新方法.
- 潜在的应用包括非线性动力学,量子热力学和时空代数.
相关概念视频
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
Types of Damping
6.7K
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...
6.7K
Problem Solving: Energy in Simple Harmonic Motion
1.4K
Simple harmonic motion (SHM) is a type of periodic motion in time and position, in which an object oscillates back and forth around an equilibrium position with a constant amplitude and frequency. In SHM, there is a continuous exchange between the potential and kinetic energy, which results in the oscillation of the object.
Consider the spring in a shock absorber of a car. The spring attached to the wheel executes simple harmonic motion while the car is moving on a bumpy road. The force on the...
Consider the spring in a shock absorber of a car. The spring attached to the wheel executes simple harmonic motion while the car is moving on a bumpy road. The force on the...
1.4K
Energy in Simple Harmonic Motion
9.3K
To determine the energy of a simple harmonic oscillator, consider all the forms of energy it can have during its simple harmonic motion. According to Hooke's Law, the energy stored during the compression/stretching of a string in a simple harmonic oscillator is potential energy. As the simple harmonic oscillator has no dissipative forces, it also possesses kinetic energy. In the presence of conservative forces, both energies can interconvert during oscillation, but the total energy remains...
9.3K
Characteristics of Simple Harmonic Motion
13.5K
The key characteristic of the simple harmonic motion is that the acceleration of the system and, therefore, the net force are proportional to the displacement and act in the opposite direction to the displacement. Additionally, the period and frequency of a simple harmonic oscillator are independent of its amplitude. For example, diving boards move faster or slower based on their thickness. A stiff, thick diving board has a large force constant, which causes it to have a smaller period, while a...
13.5K
Forced Oscillations
6.8K
When an oscillator is forced with a periodic driving force, the motion may seem chaotic. The motions of such oscillators are known as transients. After the transients die out, the oscillator reaches a steady state, where the motion is periodic, and the displacement is determined.
6.8K


