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相关概念视频

Forced Oscillations01:06

Forced Oscillations

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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.
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Entropy Change in Reversible Processes01:10

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In the Carnot engine, which achieves the maximum efficiency between two reservoirs of fixed temperatures, the total change in entropy is zero. The observation can be generalized by considering any reversible cyclic process consisting of many Carnot cycles. Thus, it can be stated that the total entropy change of any ideal reversible cycle is zero.
The statement can be further generalized to prove that entropy is a state function. Take a cyclic process between any two points on a p-V diagram.
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Damped Oscillations01:07

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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...
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Types of Damping01:20

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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...
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Oscillations about an Equilibrium Position01:04

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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...
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Atomic Nuclei: Nuclear Relaxation Processes01:23

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In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis.
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噪音引起的混乱:一种有条件的随机动态视角.

Bernat Bassols-Cornudella1, Jeroen S W Lamb1,2,3

  • 1Department of Mathematics, Imperial College London, London SW7 2AZ, United Kingdom.

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概括

噪音可以在随机动态系统中意外造成混乱. 这项研究表明,在一个隔间模型中,即使噪音水平很高,预期逃跑时间的快速减少也会导致混乱.

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科学领域:

  • * 复杂的系统 * 复杂的系统
  • * 非线性动力学
  • * 混沌理论 *

背景情况:

  • * 在随机动态系统中理解过渡到混沌至关重要.
  • *现有的文献通常依赖于小噪声假设或确定性模型.
  • *噪音振幅在制造混乱中的作用需要进一步研究.

研究的目的:

  • * 分析噪音诱导的混乱转换在一个有边界的附加噪音的物流图.
  • * 开发一个框架来分析混乱的出现,而不是小噪音的假设.
  • * 确定导致噪音引起的混乱的关键机制.

主要方法:

  • * 利用有条件的随机动力学来分析系统.
  • *使用预期逃跑时间和条件的利亚普诺夫指数.
  • * 开发了一个分区模型,表示竞争动态.

主要成果:

  • * 随着噪声振幅的增加,证明了混乱的出现 (正的利亚普诺夫指数).
  • * 确定了从收缩中预期逃脱时间的快速衰减作为主要驱动因素.
  • * 观察到其他订单参数在过渡期间基本保持不变.

结论:

  • * 噪音诱导的混乱转变可以使用有条件的随机动态有效地分析.
  • * 这项研究提供了一种独立于小噪声假设的新方法.
  • *预期逃脱时间的衰减是这个模型中出现混乱的关键指标.