一般化运输的热力学边界:从单分子到散装可观测物
1Mathematical bioPhysics Group, <a href="https://ror.org/03e76ya46">Max Planck Institute for Multidisciplinary Sciences</a>, 37077 Göttingen, Germany.
Physical review letters
|August 23, 2024
概括
我们为在不平衡系统中可观测的运输建立了一个通用的速度限制. 这种热力学成本约束适用于随机和决定性动力学,有助于批量实验分析.
科学领域:
- 统计力学 统计力学
- 热力学是一种热力学.
- 非平衡的系统是不平衡的.
背景情况:
- 随机热力学描述了具有波动动力的系统.
- 对可观测物进行传输对于理解系统行为至关重要.
- 当前的方法经常与大量实验和低压动力学作斗争.
研究的目的:
- 为在d维非平衡系统中运输可微分标尺可观测的物建立一个通用上限.
- 为了将随机热力学与大量实验观测联系起来.
- 为了弥合热力学推理对表现出低压动态的系统的差距.
主要方法:
- 导出一个时间集成的通用速度限制.
- 理论分析各种动态系统中的运输界限.
- 使用示例,展示对大量实验的适用性.
主要成果:
- 任何可观测的可微分标量体的传输都受到由坐标拉伸缩的总产量所限制.
- 这一边界统一了低压,过压的随机和决定性动态.
- 边界依赖于平均值,而不是波动,这使得它适用于批量测量.
结论:
- 导出运输边界为各种系统中的热力学推理提供了一个实用的工具.
- 它有助于从大量观测中研究分子机器和其他系统.
- 这项工作增强了随机热力学对现实世界实验的适用性.
相关概念视频
Reynolds Transport Theorem
1.1K
The Reynolds transport theorem provides a framework to relate the time rate of change of an extensive property within a system to that in a control volume, which is crucial for analyzing fluid dynamics. Extensive properties, such as mass, velocity, acceleration, temperature, and momentum, can be expressed in terms of the mass of a fluid portion. These properties are called extensive because they depend on the system's size, while intensive properties are their corresponding values per unit...
1.1K
Distribution of Molecular Speeds
3.9K
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...
3.9K
Kinetic Molecular Theory: Molecular Velocities, Temperature, and Kinetic Energy
27.4K
The kinetic molecular theory qualitatively explains the behaviors described by the various gas laws. The postulates of this theory may be applied in a more quantitative fashion to derive these individual laws.
27.4K
Zeroth Law of Thermodynamics
4.9K
Experimentally, if object A is in equilibrium with object B, and object B is in equilibrium with object C, then object A is in equilibrium with object C. That statement of transitivity is called the "zeroth law of thermodynamics." For example, a cold metal block and a hot metal block are both placed on a metal plate at room temperature. Eventually, the cold block and the plate will be in thermal equilibrium. In addition, the hot block and the plate will be in thermal equilibrium.
4.9K
Entropy
29.1K
Salt particles that have dissolved in water never spontaneously come back together in solution to reform solid particles. Moreover, a gas that has expanded in a vacuum remains dispersed and never spontaneously reassembles. The unidirectional nature of these phenomena is the result of a thermodynamic state function called entropy (S). Entropy is the measure of the extent to which the energy is dispersed throughout a system, or in other words, it is proportional to the degree of disorder of a...
29.1K
Second Law of Thermodynamics
23.4K
In the quest to identify a property that may reliably predict the spontaneity of a process, a promising candidate has been identified: entropy. Processes that involve an increase in entropy of the system (ΔS > 0) are very often spontaneous; however, examples to the contrary are plentiful. By expanding consideration of entropy changes to include the surroundings, a significant conclusion regarding the relation between this property and spontaneity may be reached. In thermodynamic...
23.4K


