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Stirling Cycle: In Stirling cycle, Carnot cycle's compression and expansion isentropic processes are replaced by two constant-volume regeneration processes. During the regeneration process heat is transferred to a thermal storage device i.e. regenerator during one part and is transferred back to the working fluid in another part of the cycle. The cycle consist of 4 different processes namely: Isothermal expansion process (1-2): During this heat addition from external source takes place. • Constant volume heat transfer (2-3): During this internal heat transfer from gas to regenerator takes place. • Isothermal compression (3-4): During this heat rejection to the external sink takes place. • Constant volume heat transfer (4-1): During this internal heat transfer from the regenerator to the gas takes place. T P Q TH 1 Q 2 v=const. Qram TH=const. v-const 2 4 TL 3 4 Qout Qout 3 TL =const. Advantages: . Few moving parts.
Limiting wear on components. • Low emissions of NOx and unburned fuel. . Fuel versatility. Disadvantages: . High cost and reliability issues. . Low electrical efficiency. Performance, Efficiency and Suitability: . Stirling cycle has high theoretical efficiencies. . Current operational efficiencies of Stirling cycle is around 12 to 20 percent, due to material and design limitations. • Stirling engines are suitable for residential or portable applications. The small size and quiet operation means that they would integrate well into a domestic environment. • The high costs and small size of Stirling engines limits the applicability of this technology in developing regions.
woneral Ericsson Cycle: The Ericsson cycle is an altered version of the Carnot cycle in which the two isentropic processes featured in the Carnot cycle are replaced by two constant-pressure regeneration processes. The cycle consist of 4 different processes namely: Isothermal expansion process. . Constant pressure or isobaric heat rejection process. . Isothermal compression process. . Constant pressure or isobaric heat absorption process. TETA Pressure sother hermal Temperature Constant Pressure Constant Pressure Volume Entropy • The theoretical efficiencies of both, Ericsson and Stirling cycles acting in the same limits are equal to the Carnot efficiency for same limits. Brayton Cycle: According to the principle of the Brayton cycle, air is compressed in the turbine compressor. The air is then mixed with fuel, and burned under constant pressure conditions in the combustor. The resulting hot gas is allowed to expand through a turbine to perform work. The Brayton cycle consists of four basic processes: Isentropic compression process.
. Constant pressure heat addition process. Isentropic expansion process. Constant pressure heat rejection process. P 3 S = const S=const. A 3 T P=const. 1 P=const. Advantages: . It has great reliability especially where power output required is high. . It requires low cost and consumption of lubricating oil. . It can make use of different forms of fuel ranging from synthetic oil to natural oil.
. It emits low toxic emission. Dis-advantages: It is less efficient than the reciprocating engines. It is less responsive to demand of change in power.