热力学系统和第一定律

J. Ansermet, S. Brechet
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引用次数: 0

摘要

热力学系统的定义包括其外壳的特征。系统可以是封闭的或开放的,绝热的或非热的,刚性的或可移动的。状态变量可以是广泛的,也可以是密集的。状态函数只是状态变量的函数。一个系统可以被隔墙分隔成子系统,隔墙可以是不渗透的或渗透的,可以是绝热的或非绝热的,可以是固定的或可移动的。系统的状态可能因机械过程或热过程而改变,从而引起热传递、传质或做功。热力学第一定律是用包括动能在内的总能量来表示的,这样就可以分析热力学系统,在经典力学和热力学之间建立了概念上的联系。通过在热力学的框架下考察阻尼谐振子,揭示了对非机械状态变量的需要。
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Thermodynamic System and First Law
The definition of a thermodynamic system includes the characterisation of its enclosure. The system can be closed or open, adiabatic or diathermal, rigid or mobile. State variables may be extensive or intensive. State functions are functions of the state variables only. A system may be divided into subsystems separated by walls that can be impermeable or permeable, adiabatic or diathermal, fixed or mobile. The state of a system may be changed by mechanical processes or thermal processes, resulting in a thermal transfer, mass transfer or work. The first law is expressed in terms of the total energy that includes the kinetic energy, so that thermomechanical systems can be analysed, creating a conceptual link between classical mechanics and thermodynamics. By examining a damped harmonic oscillator in the framework of thermodynamics, the need for a non-mechanical state variable is revealed.
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