In: Mechanical Engineering
Explain the Carnot engine cycle and plot its process on a) T-S diagram b) p-v diagram
The Carnot engine is an ideal engine. consist of 4 ideal reversible processes: The cycle was first proposed by a French Scientist Sadi Carnot.
Consider a closed system that consists of a gas contained in an adiabatic piston-cylinder device. The insulation of the cylinder head is such that it may be removed to bring the cylinder into contact with reservoirs to provide heat transfer.
The four reversible processes are as follows:
1-2: Constant Temperature (Isothermal) Expansion:
Initially (state 1), the
temperature of the gas is TH and the cylinder head is in
close contact with a source at temperature TH. The gas
is allowed to expand slowly, doing work on the surroundings. As the
gas expands, the temperature of the gas tends to decrease. But as
soon as the temperature drops by an infinitesimal amount dT, some
heat is transferred from the reservoir into the gas, raising the
gas temperature to TH. Thus, the gas temperature is kept
constant at TH. Since the temperature difference between
the gas and the reservoir never exceeds a differential amount dT,
this is a reversible
heat transfer process. It continues until the piston reaches
position 2. The amount of total heat transferred to the gas during
this process is QH.
2-3: Reversible Adiabatic (Isentropic) Expansion
At state 2, the reservoir that was in contact with the cylinder head is removed and replaced by insulation so that the system becomes adiabatic. The gas continues to expand slowly, doing work on the surroundings until its temperature drops from TH to TL (state 3). The piston is assumed to be frictionless and the process to be quasi-equilibrium, so the process is reversible as well as adiabatic.
3-4: Constant Temperature (Isothermal) Compression
At state 3, the insulation at the cylinder head is removed, and the cylinder is brought into contact with a sink at temperature TL. Now the piston is pushed inward by an external force, doing work on the gas. As the gas is compressed, its temperature tends to rise. But as soon as it rises by an infinitesimal amount dT, heat is transferred from the gas to the sink, causing the gas temperature to drop to TL. Thus, the gas temperature remains constant at TL. Since the temperature difference between the gas and the sink never exceeds a differential amount dT, this is a reversible heat transfer process. It continues until the piston reaches state 4. The amount of heat rejected from the gas during this process is QL.
4-1: Reversible Adiabatic (Isentropic) Compression
State 4 is such that when the
low-temperature reservoir is removed, the insulation is put back on
the cylinder head, and the gas is compressed in a reversible
manner, the gas returns to its initial state
(state 1). The temperature rises from TL to
TH during this reversible adiabatic compression process,
which completes the cycle.
P-v diagram
T-s diagram: