Gas power cycles are essential in thermodynamics, converting heat into work. Stirling and Ericsson cycles stand out for their unique features, using closed systems and regenerators to improve efficiency. They offer interesting alternatives to traditional internal combustion engines.
These cycles use isothermal and isochoric/isobaric processes to maximize . While they have high theoretical efficiencies, practical limitations affect their real-world performance. Understanding these cycles deepens our knowledge of thermodynamic principles and their applications.
Stirling and Ericsson Cycles
Principles and Components
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Operate using a working fluid (air, helium, or hydrogen) that remains within the system
Consist of four thermodynamic processes: , , , and ()
Comprise two isothermal processes (compression and expansion) and two isobaric processes (heat addition and rejection) ()
Utilize a to store and transfer heat between the hot and cold sides of the engine, improving
Engine Components
Include a cylinder, two pistons (a power piston and a displacer piston), a regenerator, and heat exchangers for heat addition and rejection (Stirling engine)
Contain a cylinder, a piston, a displacer, a regenerator, and heat exchangers for heat addition and rejection (Ericsson engine)
Thermodynamic Processes in Cycles
Stirling Cycle Processes
Isothermal compression occurs at a constant low temperature, with heat being rejected to the external sink
Isochoric heat addition involves the transfer of heat from the regenerator to the working fluid at a constant volume
Isothermal expansion occurs at a constant high temperature, with heat being added to the working fluid from an external source
Isochoric heat rejection involves the transfer of heat from the working fluid to the regenerator at a constant volume
Ericsson Cycle Processes
Isothermal compression occurs at a constant low temperature, with heat being rejected to the external sink
involves the transfer of heat from an external source to the working fluid at a constant pressure
Isothermal expansion occurs at a constant high temperature, with heat being added to the working fluid from an external source
involves the transfer of heat from the working fluid to the external sink at a constant pressure
Stirling vs Other Gas Cycles
Advantages of Stirling and Ericsson Cycles
Have higher theoretical thermal efficiencies compared to other gas power cycles (Otto and Diesel cycles) due to their regenerative nature and the use of isothermal processes
Allow for the use of various heat sources (solar energy, geothermal energy, and waste heat) due to their closed-cycle nature, making them more versatile than open-cycle engines
Produce lower noise and vibration levels compared to internal combustion engines, as they do not involve explosive combustion processes
Result in lower emissions compared to internal combustion engines, as the combustion process is separated from the working fluid
Disadvantages of Stirling and Ericsson Cycles
Have lower power-to-weight ratios compared to internal combustion engines, making them less suitable for mobile applications (automobiles, aircraft)
Increase complexity and cost compared to other gas power cycles due to the presence of a regenerator
Can result in slower response times to load changes compared to internal combustion engines due to heat transfer limitations
Efficiency and Work Output of Cycles
Thermal Efficiency Calculation
Given by the ratio of the net work output to the : η=Wnet/Qin
Equal to the for an ideal Stirling or Ericsson cycle: η=1−(Tc/Th), where Tc is the low temperature and Th is the high temperature
Lower than the ideal values due to various irreversibilities (heat transfer limitations, friction, and pressure drops)
Work Output Calculation
Determined by multiplying the net work output per cycle (Wnet) by the number of cycles per unit time (N): Power=Wnet×N
Net work output (Wnet) is the difference between the work done by the engine during expansion (Wexp) and the work done on the engine during compression (Wcomp): Wnet=Wexp−Wcomp
Calculated by determining the work done during each process using the appropriate thermodynamic equations for isothermal, isochoric, or isobaric processes, and then summing the work values
Lower than the ideal values due to various irreversibilities (heat transfer limitations, friction, and pressure drops)