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Lecture 02 Carnot Cycle

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Heat Engine
Fig. 6.9 Part of the heat received by a heat engine is converted to work,
while the rest is rejected to a sink
Heat Engines
• They receive heat from a high-temperature source.
• They convert part of this heat to work.
• They reject the remaining waste heat to a lowtemperature sink.
• They operate on a cycle.
Fig 6.10 Schematic of a steam power plant
Fig 6.11 A portion of the work output of a heat engine is consumed
internally to maintain continuous operation
• Thermal Efficiency
(7.3)
Reversible and Irreversible Processes
• Reversible process: is defined as a process that can
be reversed without leaving any trace on the
surroundings.
• Processes that are not reversible are called
irreversible processes.
• Reasons:
The Carnot Cycle
The best known reversible cycle is the Carnot cycle
Reversible isothermal expansion (Process 1-2,
TH = constant)
Reversible adiabatic expansion (Process 2-3)
Reversible isothermal compression (Process 3-4,
TL= constant
Reversible adiabatic compression (Process 4-1)
Fig 6.36 Execution
of ofthe
Carnot
insystem
a closed system
6.37 Execution
the Carnot
cyclecycle
in a closed
Fig 6.37 P-V diagram of the Carnot cycle
Fig 6.38 P-V diagram of the reversed Carnot cycle
The Carnot Principles
1.
The efficiency of an irreversible heat engine is always less
than the efficiency of a reversible one operating between the
same two reservoirs.
2. The efficiencies of all reversible heat engines operating
between the same two reservoirs are the same.
Fig 6.39 The Carnot principles
The Carnot Heat Engine
Fig 6.45 The Carnot heat engine is the most efficient of all heat engines
operating between the same high and low temperature reservoirs.
Fig 6.46 No heat engine can have a higher efficiency than a reversible heat engine
operating between the same high and low temperature reservoirs
Fig 6.48 The fraction of heat that can be converted to work as a
function of source temperature (for TL = 303 K)
7.11 The Carnot Refrigerator and Heat Pump
Fig 6.50 No refrigerator can have a higher COP than a reversible
refrigerator operating between the same temperature limits
Reference:
Thermodynamics: An Engineering Approach
By Y. Cengel, M.A. Boles, McGraW Hill.
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