Following are the four processes of Carnot cycle:
In (a), the process is reversible isothermal gas expansion. In this process, the amount of heat absorbed by the ideal gas is qin from the heat source which is at a temperature of Th. The gas expands and does work on the surroundings.
In (b), the process is reversible adiabatic gas expansion. Here, the system is thermally insulated and the gas continues to expand and work is done on the surroundings. Now the temperature is lower, TI.
In (c), the process is reversible isothermal gas compression process. Here, the heat loss, qout occurs when the surroundings do the work at temperature TI.
In (d), the process is reversible adiabatic gas compression. Again the system is thermally insulated. The temperature again rise back to Th as the surrounding continue to do their work on the gas.
Step 1:
Isothermal expansion: The gas is taken from P1, V1, T1 to P2, V2 ,T2. Heat Q1 is absorbed from the reservoir at temperature T1. Since the expansion is isothermal, the total change in internal energy is zero and the heat absorbed by the gas is equal to the work done by the gas on the environment, which is given as:
W1→2=Q1=μ×R×T1×ln(v2/v1)
Step 2:
Adiabatic expansion: The gas expands adiabatically from P2, V2, T1 to P3, V3, T2.
Here work done by the gas is given by:
W2→3={μR/(γ−1)}*(T1−T2)
Step 3:
Isothermal compression: The gas is compressed isothermally from the state (P3, V3, T2) to (P4, V4, T2).
Here, the work done on the gas by the environment is given by:
W3→4=μRT2ln(v3/v4)
Step 4:
Adiabatic compression: The gas is compressed adiabatically from the state (P4, V4, T2) to (P1, V1, T1).
Here, the work done on the gas by the environment is given by:
W4→1={μR/(γ−1)}*(T1−T2)
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