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 TH v=const. 2 Qin QRE Th=const. v=const. Qres 3 4 TL 4 Qout Qout ذرا 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.
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.
T3=T4 Isothermal Pressure Isothermal Temperature Constant Pressure Constant Pressure T2=1 2 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 2 3 S = const. S = const. 4 T P =const. N 4 P=const. S
Advantages:
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