SECOND LAW OF THERMODYNAMICS
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1 SECOND LAW OF THERMODYNAMICS
2 2 ND Law of Thermodynamics Puts a limitation on the conversion of some forms of energy Determines the scope of an energy conversion and if an energy conversion is possible Provides means of evaluating the thermodynamic performance of systems and processes so that sound design decisions can be made
3 KELVIN-PLANCK STATEMENT
4 Kelvin-Planck Statement of the 2 nd Law It is impossible to construct a heat engine that operates in a cycle, receives a high-temperature body, and does an equal amount of work. This implies that it is impossible to build a heat engine that has a thermal efficiency of 100%. The thermal efficiency of practical heat engines typically ranges from 10 to 40%. Thus in practice, some portion of the heat supplied from a high-temperature source is always rejected to a low-temperature sink.
5 TWO PRINCIPLES DRAWN FROM KELVIN-PLANCK STATEMENT
6 Two Principles drawn from Kelvin-Planck Statement 1. Cycle efficiency of an irreversible power cycle is always less than the cycle efficiency of a reversible power cycle when each operates between the same reservoirs 2. All reversible power cycles operating between the same two thermal reservoirs have the same cycle efficiency. It implies that the specific states, working fluid, or specific processes of the reversible power cycle do not affect the cycle efficiency.
7 Reversible Process Process that can be reversed and leaves no change in either system or surroundings. Internally reversible process Process in which the system can be returned to its initial equilibrium state without leaving any permanent changes in the system Totally reversible process Process in which both system and its surroundings must be capable of being returned to their initial equilibrium states without leaving any permanent changes in both the system and surroundings
8 Irreversibility Representing a loss of work A process is called irreversible if the system and all the parts of its surrounding cannot be exactly restored to their respective initial states after the process has occurred.
9 Common Causes of Irreversibility 1. Electric Resistance 2. Inelastic Deformation 3. Viscous flow of a fluid 4. Solid-solid friction 5. Heat transfer from a finite temperature difference 6. Fluid flow through valves and porous plugs 7. Mixing of Dissimilar gases or liquids 8. Mixing of identical fluids initially at different pressures and temperatures
10 Thermal efficiency Ratio of output (the energy sought) to the input (the energy supplied) Thermal Reservoir Body to which and from which heat can be transferred indefinitely without a change in its temperature e.g. atmosphere, oceans, and lakes
11 CARNOT CYCLE
12 Carnot Cycle The most efficient cycle that can operate between two constant-temperature reservoirs A totally reversible cycle Named after the French engineer, Nicolas Leonard Sadi Carnot
13 Carnot Heat Engine Thermal efficiency: th W T T Q T net H L input H * Carnot Ideal Actual th th th
14 Example A heat engine operates on the Carnot cycle. It produces 50 kw of power while operating between limits of 800 C and 100 C. Determine the engine efficiency and the amount of heat added.
15 CLAUSIUS STATEMENT OF THE SECOND LAW
16 Clausius Statement of the Second Law States that it is impossible to construct a refrigerator that operates without an input of work. Simply means that heat cannot flow by itself from a low temperature to a high temperature
17 REVERSE CARNOT CYCLE
18 Carnot Refrigerator Coefficient of Performance (COP) COP QL TL W T T net H L *Reverse Carnot COP>Ideal COP>Actual COP
19 Example A refrigerator maintains the cooled space at 2 C when the ambient air around the refrigerator is 25 C. The refrigerator has a coefficient of performance of 2.5. The rate of cooling in the refrigerated space is 8000 kj/hr. a) Determine the power consumption and the heat-transfer rate b) Suppose the refrigerator with a Carnot refrigerator, determine its COP
SECOND LAW OF THERMODYNAMICS
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