具有较小外部不可逆性的热电器件的最佳性能
Rajeshree Chakraborty1, Ramandeep S Johal1
1Indian Institute of Science Education and Research Mohali, Department of Physical Sciences, Sector 81, S.A.S. Nagar, Manauli PO 140306, Punjab, India.
Physical review. E
|October 21, 2025
概括
这项研究将内部和外部不可逆向性整合到热电装置分析中,在最大功率 (EMP) 表达下产生新的效率. 这些发现为了解热电发电机和冰箱性能提供了一个统一的框架.
科学领域:
- 热力学是一种热力学.
- 材料科学 材料科学 材料科学
- 能源转换 能源转换
背景情况:
- 热电设备的传统热力学分析往往简化了不可逆性,专注于内部或外部因素.
- 现有的最大功率效率 (EMP) 模型,如内向可逆和外向可逆,通过只解决特定不可逆性的问题,提供了有限的范围.
研究的目的:
- 开发一个统一的热力学模型,同时结合热电器件的内部和外部不可逆性.
- 在对称和小的外部不可逆性近似下,为最大功率 (EMP) 的效率推导出可处理的表达式.
- 探索这种统一模型对热电发电机和冰箱的影响,包括与现有理论和模型进行比较.
主要方法:
- 在常量属性框架内开发了一个热力学模型来分析热电设备.
- 集成的同时内部和外部不可逆性,采用对称和小外部不可逆性的近似值.
- 从关键参数 (热导电比率,材料价值数字和温度比率) 导出了最大功率 (EMP) 的效率的分析表达式.
- 将衍生的EMP与精确模型和其他有限时间热力学不可逆转模型进行比较.
- 将分析扩展到热电冰箱,以研究最大冷却功率的效率.
主要成果:
- 获得了最大功率效率 (EMP) 的可处理表达式,该表达式考虑了内部和外部不可逆性.
- 证明了在可逆近似的热电发生器 (TEG) 可以在高温状态下映射到费曼杆模型中.
- 提供了一个关于热电器件和介视模型之间的关系的替代视角.
- 在类似的假设下,分析了热电冰箱在最大冷却功率的效率.
结论:
- 开发的模型通过整合多种不可逆性的方法,提供了对热电器件性能更全面的了解.
- 这些发现为分析热电发电机和冰箱提供了一个统一的框架.
- 这项研究为宏观热电现象与微观模型 (如费曼子) 之间的联系提供了新的见解.
更多相关视频
相关概念视频
The Carnot Cycle and the Second Law of Thermodynamics
3.7K
The Carnot engine works between two heat reservoirs of fixed temperatures. The Carnot cycle begs the following question: Is it possible to devise a heat engine that is more efficient than a Carnot engine between two fixed temperatures? The answer lies in designing a Carnot refrigerator.
Since the individual steps in a Carnot cycle can be reversed, the entire cycle is, thus, reversible. If a Carnot cycle is reversed, it becomes a Carnot refrigerator. It extracts heat Qc from a cold reservoir at...
Since the individual steps in a Carnot cycle can be reversed, the entire cycle is, thus, reversible. If a Carnot cycle is reversed, it becomes a Carnot refrigerator. It extracts heat Qc from a cold reservoir at...
3.7K
The Carnot Cycle
4.0K
Converting work to heat is an irreversible process, and the purpose of a heat engine is to reverse the effect partially. Heat engines aim to increase the efficiency of the reversal, that is, maximize the work retrieved from heat. If the efficiency of a heat engine were 100%, it would imply reversing the process completely without introducing any other effect. Thus, it would violate the second law of thermodynamics.
What could be the theoretical limit to the efficiency of a heat engine? The...
What could be the theoretical limit to the efficiency of a heat engine? The...
4.0K
Reversible and Irreversible Processes
5.6K
The thermodynamic processes can be classified into reversible and irreversible processes. The processes that can be restored to their initial state are called reversible processes. It is only possible if the process is in quasi-static equilibrium, i.e., it takes place in infinitesimally small steps, and the system remains at equilibrium However, these are ideal processes and do not occur naturally. An ideal system undergoing a reversible process is always in thermodynamic equilibrium within...
5.6K
Entropy
3.5K
The first law of thermodynamics is quantitatively formulated via an equation relating the internal energy of a system, the heat exchanged by it, and the work done on it. A quantitative formulation of the second law of thermodynamics leads to defining a state function, the entropy.
When an ideal gas expands isothermally, the disorder in the gas increases. From the molecular perspective, the gas molecules have more volume to move around in.
Consider an infinitesimal step in the expansion, which...
When an ideal gas expands isothermally, the disorder in the gas increases. From the molecular perspective, the gas molecules have more volume to move around in.
Consider an infinitesimal step in the expansion, which...
3.5K
Statements of the Second Law of Thermodynamics
4.9K
The second law of thermodynamics can be stated in several different ways, and all of them can be shown to imply the others. The Clausius’ statement of the second law of thermodynamics is based on the irreversibility of spontaneous heat flow. It states that heat will not flow from the colder body to the hotter body unless some other process is involved. Additionally, as per the Kelvin’s statement, it is impossible to convert the heat from a single source into work without any other...
4.9K
Efficiency of The Carnot Cycle
3.6K
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...
3.6K


