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Entropy Change in Reversible Processes01:10

Entropy Change in Reversible Processes

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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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¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

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Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
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Woodward–Hoffmann Selection Rules and Microscopic Reversibility01:34

Woodward–Hoffmann Selection Rules and Microscopic Reversibility

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Electrocyclic reactions, cycloadditions, and sigmatropic rearrangements are concerted pericyclic reactions that proceed via a cyclic transition state. These reactions are stereospecific and regioselective. The stereochemistry of the products depends on the symmetry characteristics of the interacting orbitals and the reaction conditions. Accordingly, pericyclic reactions are classified as either symmetry-allowed or symmetry-forbidden. Woodward and Hoffmann presented the selection criteria for...
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Space-Time Curvature and the General Theory of Relativity01:17

Space-Time Curvature and the General Theory of Relativity

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In 1905, Albert Einstein published his special theory of relativity. According to this theory, no matter in the universe can attain a speed greater than the speed of light in a vacuum, which thus serves as the speed limit of the universe.
This has been verified in many experiments. However, space and time are no longer absolute. Two observers moving relative to one another do not agree on the length of objects or the passage of time. The mechanics of objects based on Newton's laws of...
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Distribution of Molecular Speeds01:27

Distribution of Molecular Speeds

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The motion of molecules in a gas is random in magnitude and direction for individual molecules, but a gas of many molecules has a predictable distribution of molecular speeds. This predictable distribution of molecular speeds is known as the Maxwell-Boltzmann distribution. The distribution of molecular speeds in liquids is comparable to that of gases but not identical and can help to understand the phenomenon of the boiling and vapor pressure of a liquid. Consider that a molecule requires a...
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Entropy and the Second Law of Thermodynamics01:20

Entropy and the Second Law of Thermodynamics

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The second law of thermodynamics can be stated quantitatively using the concept of entropy. Entropy is the measure of disorder of the system.
The relation  between entropy and disorder can be illustrated with the example of the phase change of ice to water. In ice, the molecules are located at specific sites giving a solid state, whereas, in a liquid form, these molecules are much freer to move. The molecular arrangement has therefore become more randomized. Although the change in average...
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相关实验视频

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Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
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Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

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量子形态驱动器中的临界缓慢的希尔伯特空间厄戈迪性.

Saúl Pilatowsky-Cameo1, Soonwon Choi1, Wen Wei Ho2,3

  • 1Massachusetts Institute of Technology, Center for Theoretical Physics, Cambridge, Massachusetts 02139, USA.

Physical review letters
|October 19, 2025
PubMed
概括

最大的原理受到非周期性驱动的挑战. 这项研究证明,由图埃-莫尔斯序列驱动的量子系统实现了强大的量子厄戈迪性,揭示了复杂量子系统中极其缓慢的动态.

科学领域:

  • 量子动力学 量子动力学是什么?
  • 统计物理 统计物理
  • 复杂的系统复杂的系统.

背景情况:

  • 最大的原理是分析复杂动态的基础.
  • 之前的研究表明,非周期性驱动,如图-莫尔斯驱动,导致非埃尔戈迪状态,挑战了这一原则.
  • 这种紧张关系源于ergodicity和新出现的nonergodic行为之间的明显冲突.

研究的目的:

  • 解决最大原则与无周期驱动器的发现之间的明显紧张关系.
  • 严格调查量子系统在Thue-Morse驱动下长期的行为.
  • 描述驱动量子系统中出现的稳定状态和保存量的性质.

主要方法:

  • 严格的数学证明来证明量子厄戈迪性.
  • 在希尔伯特空间中分析量子状态的时间演变.
  • 数字模拟用于探索各种非周期驱动下的动力学.

主要成果:

  • 图-莫尔斯驱动器导致长时间极限中的强烈形式的量子厄戈迪性.
  • 量子系统表现出极其缓慢的完整的希尔伯特空间积分,在长时间内接近Floquet驱动器.
  • 这种无尺度的ergodic动态并不仅仅是Thue-Morse驱动的特征,而是观察到其他形态序列.

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Gradient Echo Quantum Memory in Warm Atomic Vapor
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Gradient Echo Quantum Memory in Warm Atomic Vapor

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An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
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An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

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相关实验视频

Last Updated: Jan 6, 2026

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11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

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Gradient Echo Quantum Memory in Warm Atomic Vapor
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Gradient Echo Quantum Memory in Warm Atomic Vapor

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An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
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An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

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结论:

  • 这项研究通过证明在无周期驱动下可能存在的强量子厄戈迪性来解决这种紧张局面.
  • 在依赖时间的量子系统中发现了一种新的动力学类别,即临界缓慢的完整的希尔伯特空间厄戈迪性.
  • 只有在极长的时间尺度后才能达到完全的ergodicity,从而为复杂的量子动力学提供了新的见解.