Jove
Visualize
联系我们
JoVE
x logofacebook logolinkedin logoyoutube logo
关于 JoVE
概览领导团队博客JoVE 帮助中心
作者
出版流程编辑委员会范围与政策同行评审常见问题投稿
图书馆员
用户评价订阅访问资源图书馆顾问委员会常见问题
研究
JoVE JournalMethods CollectionsJoVE Encyclopedia of Experiments存档
教育
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab Manual教师资源中心教师网站
使用条款与条件
隐私政策
政策

相关概念视频

Pressure and Volume in an Adiabatic Process01:27

Pressure and Volume in an Adiabatic Process

2.7K
Free expansion of a gas is an adiabatic process. However, there are few differences between free expansion and adiabatic expansion. During free expansion, no work is done, and there is no change in internal energy. But, for an adiabatic expansion, work is done, and there is a change in internal energy. During an adiabatic process, the relation between the pressure and volume is obtained from the condition for the adiabatic process, that is, 
2.7K
Adiabatic Processes for an Ideal Gas01:18

Adiabatic Processes for an Ideal Gas

3.1K
When an ideal gas is compressed adiabatically, that is, without adding heat, work is done on it, and its temperature increases. In an adiabatic expansion, the gas does work, and its temperature drops. Adiabatic compressions actually occur in the cylinders of a car, where the compressions of the gas-air mixture take place so quickly that there is no time for the mixture to exchange heat with its environment. Nevertheless, because work is done on the mixture during the compression, its...
3.1K
Isothermal Processes01:21

Isothermal Processes

3.7K
A thermodynamic process that occurs at constant temperature is called an isothermal process. Heat slowly flows into the system or out of the system to maintain thermal equilibrium. Processes involving phase changes like water evaporation into steam or freezing water into ice at a constant temperature are examples of Isothermal Processes.
An ideal gas can also undergo isothermal expansion or compression.
For example, consider 1 mole of an ideal gas inside an isolated cylinder at initial volume V...
3.7K
Isochoric and Isobaric Processes01:21

Isochoric and Isobaric Processes

3.5K
A thermodynamic process that occurs at constant volume is called an isochoric process. According to the first law of thermodynamics, heat supplied or removed from the system is partially utilized to perform work and change the internal energy of the system. However, in an isochoric process, the volume remains constant. Hence, the work done by the system is zero. Therefore, the exchange of heat changes the internal energy of the system only. 
Suppose 1000 g of water is heated from 40...
3.5K
Work Done in an Adiabatic Process01:20

Work Done in an Adiabatic Process

3.3K
Consider the adiabatic compression of an ideal gas in the cylinder of an automobile diesel engine. The gasoline vapor is injected into the cylinder of an automobile engine when the piston is in its expanded position. The temperature, pressure, and volume of the resulting gas-air mixture are 20 °C, 1.00 x 105 N/m2, and 240 cm3 , respectively. The mixture is then compressed adiabatically to a volume of 40 cm3. Note that, in the actual operation of an automobile engine, the compression is not...
3.3K
Efficiency of The Carnot Cycle01:16

Efficiency of The Carnot Cycle

2.7K
The hypothetical Carnot cycle consists of an ideal gas subjected to two isothermal and two adiabatic processes. Since the internal energy of an ideal gas depends only on its temperature, which is the same before and after the completion of the Carnot cycle, there is no change in its internal energy. Hence, using the first law of thermodynamics, the total heat exchanged by the ideal gas equals the total work done. Thus, we can quantify the efficiency of the Carnot cycle via the heat exchanged...
2.7K

您也可能阅读

相关文章

通过共同作者、期刊和引用图与本文相关的文章。

排序
Same author

Unifying Kibble-Zurek Mechanism in Weakly Driven Processes.

Entropy (Basel, Switzerland)·2026
Same author

Minimal dissipation with viscoelastic baths in weakly driven processes.

Physical review. E·2025
Same author

Analytical shortcuts to adiabaticity of weakly driven processes.

Physical review. E·2025
Same author

Optimal work fluctuations for finite-time and weak processes.

Physical review. E·2023
Same author

Global optimization and monotonicity in entropy production of weak drivings.

Physical review. E·2023
Same author

Kibble-Zurek Scaling from Linear Response Theory.

Entropy (Basel, Switzerland)·2022

相关实验视频

Updated: Jul 23, 2025

Evolution of Staircase Structures in Diffusive Convection
07:28

Evolution of Staircase Structures in Diffusive Convection

Published on: September 5, 2018

6.6K

阿迪亚巴特过程类似于同热过程.

Pierre Nazé1

  • 1Departamento de Física, Instituto de Geociências e Ciências Exatas, Universidade Estadual Paulista "Júlio de Mesquita Filho", 13506-900, Rio Claro, SP, Brazil.

Physical review. E
|July 19, 2023
PubMed
概括

阿迪亚巴特过程与异热过程非常相似,共享热力学兼容性标准. 热隔离系统具有定义的放松时间,类似于同热系统,遵守热力学第二定律.

科学领域:

  • 热力学是一种热力学.
  • 统计力学 统计力学
  • 凝聚物质物理学 凝聚物质物理学

背景情况:

  • 附热和异热过程是基本的热力学概念.
  • 线性反应理论和热力学第二定律支配着系统的进化.
  • 了解放松时间对于描述系统动态至关重要.

研究的目的:

  • 为了证明亚底巴和同热过程之间的平行.
  • 在孤立系统中研究时间平均过度工作的热力学影响.
  • 通过线性响应理论的镜头分析兰道-泽纳模型.

主要方法:

  • 孤立和异热系统的热力学兼容性标准的比较.
  • 分析时间平均过度工作和放松功能的分析.
  • 线性响应理论应用于兰道-泽纳模型.

主要成果:

  • 对于线性反应理论与第二定律相兼容的同样的标准,适用于亚热和异热过程.
  • 对热隔离系统的明确放松时间的发现.
  • 在非单调和快速的兰道-泽纳协议中观察负生产率.

结论:

更多相关视频

Exploring the Effects of Atmospheric Forcings on Evaporation: Experimental Integration of the Atmospheric Boundary Layer and Shallow Subsurface
13:27

Exploring the Effects of Atmospheric Forcings on Evaporation: Experimental Integration of the Atmospheric Boundary Layer and Shallow Subsurface

Published on: June 8, 2015

8.8K
Experimental Methods for Investigation of Shape Memory Based Elastocaloric Cooling Processes and Model Validation
11:11

Experimental Methods for Investigation of Shape Memory Based Elastocaloric Cooling Processes and Model Validation

Published on: May 2, 2016

11.1K

相关实验视频

Last Updated: Jul 23, 2025

Evolution of Staircase Structures in Diffusive Convection
07:28

Evolution of Staircase Structures in Diffusive Convection

Published on: September 5, 2018

6.6K
Exploring the Effects of Atmospheric Forcings on Evaporation: Experimental Integration of the Atmospheric Boundary Layer and Shallow Subsurface
13:27

Exploring the Effects of Atmospheric Forcings on Evaporation: Experimental Integration of the Atmospheric Boundary Layer and Shallow Subsurface

Published on: June 8, 2015

8.8K
Experimental Methods for Investigation of Shape Memory Based Elastocaloric Cooling Processes and Model Validation
11:11

Experimental Methods for Investigation of Shape Memory Based Elastocaloric Cooling Processes and Model Validation

Published on: May 2, 2016

11.1K
  • 附热流程可以表现出与异热流程非常相似的行为.
  • 平均放松函数为理解孤立系统中的动态提供了一个一致的框架.
  • 兰道-泽纳模型在特定条件下揭示了独特的热力学行为.