Related Experiment Video
Updated: Nov 7, 2025

04:58
A Rapid Method for Modeling a Variable Cycle Engine
Published on: August 13, 2019
7.8K
Performance Analysis and Optimization for Irreversible Combined Carnot Heat Engine Working with Ideal Quantum Gases
Lingen Chen1,2, Zewei Meng3, Yanlin Ge1,2
1Institute of Thermal Science and Power Engineering, Wuhan Institute of Technology, Wuhan 430205, China.
Entropy (Basel, Switzerland)
|April 30, 2021
Summary
This study models an irreversible combined Carnot cycle using ideal quantum gases. Finite-time thermodynamics reveals optimal performance and the impact of working fluids like Fermi-Bose gas on power output.
Area of Science:
- Thermodynamics
- Quantum Mechanics
- Energy Systems Engineering
Background:
- Finite-time thermodynamics analyzes energy conversion processes under realistic constraints.
- Combined Carnot cycles offer potential for enhanced thermal efficiency and power output.
- Ideal quantum gases present unique thermodynamic properties as working fluids.
Purpose of the Study:
- To model an irreversible combined Carnot cycle using ideal quantum gases.
- To analyze the effects of thermal resistance, internal irreversibility, and heat leakage on cycle performance.
- To determine optimal operating conditions and compare different working mediums.
Main Methods:
- Developed an irreversible combined Carnot cycle model.
- Utilized finite-time thermodynamics and the quantum gas state equation.
- Employed numerical analysis and the Euler-Lagrange equation for optimization.
Main Results:
- Identified optimal working medium temperatures for maximum power output.
- Characterized performance curves: parabolic without heat leakage, loop-shaped with heat leakage.
- Demonstrated that internal irreversibility reduces both power and efficiency; heat leakage impacts efficiency only.
- Fermi-Bose gas yielded the highest power output among tested mediums.
Conclusions:
- The combined Carnot cycle's performance is significantly influenced by irreversibilities and heat leakage.
- Working medium selection, particularly ideal quantum gases like Fermi-Bose gas, is crucial for maximizing power output.
- Optimal operating conditions exist for balancing power and efficiency in these advanced thermodynamic cycles.
Keywords:
Carnot heat enginefinite-time thermodynamicsideal quantum gasirreversible combined cyclepower outputthermal efficiencyMore Related Videos
Related Concept Videos
The Carnot Cycle
3.4K
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...
3.4K
Efficiency of The Carnot Cycle
3.1K
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...
3.1K
The Carnot Cycle and the Second Law of Thermodynamics
3.1K
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...
3.1K
Path Between Thermodynamics States
3.6K
Consider the two thermodynamic processes involving an ideal gas that are represented by paths AC and ABC in Figure 1:
3.6K
Entropy
3.1K
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...
3.1K
Heat Engines
3.3K
A heat engine is a device used to extract heat from a source and then convert it into mechanical work used for various applications. For example, a steam engine on an old-style train can produce the work needed for driving the train.
Whenever we consider heat engines (and associated devices such as refrigerators and heat pumps), we do not use the standard sign convention for heat and work. For convenience, we assume that the symbols Qh, Qc, and W represent only the amounts of heat transferred...
Whenever we consider heat engines (and associated devices such as refrigerators and heat pumps), we do not use the standard sign convention for heat and work. For convenience, we assume that the symbols Qh, Qc, and W represent only the amounts of heat transferred...
3.3K

