非添加式热形式和连续和离散概率的进化方程
Evaldo M F Curado1, Fernando D Nobre1
1Centro Brasileiro de Pesquisas Físicas and National Institute of Science and Technology for Complex Systems Rua Xavier Sigaud 150, Urca, Rio de Janeiro 22290-180, Brazil.
Entropy (Basel, Switzerland)
|August 26, 2023
概括
本研究探讨了复杂系统的非添加性和它们的时间演变. 它证明了连续和离散概率的H定理,将系统进化与平衡状态和热力学定律联系起来.
科学领域:
- 统计力学 统计力学
- 复杂系统理论 复杂系统理论
- 非平衡的热力学 热力学
背景情况:
- 对复杂系统的非添加式热形式越来越感兴趣.
- 形形式依赖于概率,影响它们的时间演变.
- 需要了解非添加性的时间演变和平衡性质.
研究的目的:
- 为了研究连续和离散概率的非加法的时间演变.
- 建立非线性福克-普朗克/马斯特方程和一般的形之间的联系.
- 分析热力学含义,包括H定理,卡诺循环和热力学第三定律.
主要方法:
- 使用非线性福克-普朗克方程开发和证明连续概率的H定理.
- 开发和证明一个H定理的离散概率使用主方程.
- 连接进化方程的静态状态解决方案与来自热带极端化的平衡解决方案.
主要成果:
- 证明了福克-普朗克和主方程的静态状态解决方案与来自极极化的平衡解决方案一致.
- 证明了连续和离散概率情况的H定理,确保系统向平衡方向演变.
- 确定了卡诺特循环对一般的形态的有效性,并讨论了对非添加的热力学第三定律.
结论:
- 这项研究证实了系统进化方程与非添加形式的极化之间的基本联系.
- 物理后果包括对卡诺循环的限制和热力学第三定律的概括.
- 这些发现提供了对复杂系统中的非增值和它们的热力学行为的更深入的理解.
相关概念视频
Entropy Change in Reversible Processes
2.6K
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.
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.
2.6K
Entropy
30.3K
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...
30.3K
Entropy and the Second Law of Thermodynamics
2.9K
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...
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...
2.9K
The Second Law of Thermodynamics
5.4K
In the quest to identify a property that may reliably predict the spontaneity of a process, a promising candidate has been identified: entropy. Scientists refer to the measure of randomness or disorder within a system as entropy. High entropy means high disorder and low energy. To better understand entropy, think of a student’s bedroom. If no energy or work were put into it, the room would quickly become messy. It would exist in a very disordered state, one of high entropy. Energy must be...
5.4K
Second Law of Thermodynamics
23.9K
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...
23.9K
Third Law of Thermodynamics
19.0K
A pure, perfectly crystalline solid possessing no kinetic energy (that is, at a temperature of absolute zero, 0 K) may be described by a single microstate, as its purity, perfect crystallinity,and complete lack of motion means there is but one possible location for each identical atom or molecule comprising the crystal (W = 1). According to the Boltzmann equation, the entropy of this system is zero.
19.0K


