Presentation on theme: "AH 13-03-2010. Objectives Introduce the second law of thermodynamics. Discuss thermal energy reservoirs, reversible and irreversible processes, heat engines,"— Presentation transcript:
Objectives Introduce the second law of thermodynamics. Discuss thermal energy reservoirs, reversible and irreversible processes, heat engines, refrigerators, and heat pumps. Describe the Kelvin–Planck and Clausius statements of the second law of thermodynamics. Apply the second law of thermodynamics to cycles and cyclic devices. Describe the Carnot cycle. Examine the Carnot principles, idealized Carnot heat engines, refrigerators, and heat pumps. Determine the expressions for the thermal efficiencies and coefficients of performance for reversible heat engines, heat pumps, and refrigerators.
Conclution from Ch. IV: that a process must satisfy the first law to occur. However, satisfying the first law alone does not ensure that the process will actually take place. Example: Hot coffee; heating resistance, paddle wheel.
Kesimpulan: Proses terjadi dalam arah tertentu Proses terjadi jika memenuhi hk. I dan II Second law of thermodynamics by Clausius (1822 – 1888): Heat flows naturally from a hot object to a cold object; heat will not flow spontaneously from a cold object to a hot object.
THERMAL ENERGY RESERVOIRS We need : a hypothetical body with a relatively large thermal energy capacity (mass specific heat) that can supply or absorb finite amounts of heat without undergoing any change in temperature: thermal energy reservoir, heat reservoirs or reservoir.
Source and Sink A reservoir that supplies energy in the form of heat is called a source. one that absorbs: sink
HEAT ENGINES Work can easily be converted to other forms of energy (ex: heat) Converting other forms of energy to work is not easy. Need special devices call HEAT ENGINES
Heat Engines (Mesin Kalor) Heat engines is characterized by : 1. They receive heat from a high- temperature source (solar energy, oil furnace, nuclear reactor, etc.). 2. They convert part of this heat to work (usually in the form of a rotating shaft). 3. They reject the remaining waste heat to a low-temperature sink (the atmosphere, rivers, etc.). 4. They operate on a cycle. Heat engines involve a fluid to and from which heat is transferred while undergoing a cycle. This fluid is called the working fluid.
Steam power plant (PLTU) The work-producing device that best fits into the definition of a heat engine is the steam power plant. The various quantities involve in steam power plant are: Q in = amount of heat supplied to steam in boiler from a high-temperature source (furnace) Q out = amount of heat rejected from steam in condenser to a lowtemperature sink (the atmosphere, a river, etc.) W out = amount of work delivered by steam as it expands in turbine W in = amount of work required to compress water to boiler pressure
Net work output The net work output of this power plant is simply: W net,out = W out – W in (kJ) For a closed system undergoing a cycle, the change in internal energy U is zero, and therefore: W net,out = Q in – Q out (kJ)
Thermal Efficiency Q out is never zero; thus, the net work output of a heat engine is always less than the amount of heat input (Q in ). The fraction of the heat input that is converted to net work output is a measure of the performance of a heat engine and is called the thermal efficiency ( th )
Thermal efficiency Other expression:
T H, T L, Q H and Q L Cyclic devices (heat engines, refrigerators, and heat pumps) operate between a high-temperature medium (or reservoir) at temperature T H and a low- temperature medium (or reservoir) at temperature T L. We define these two quantities: Q H = magnitude of heat transfer between the cyclic device and the high temperature medium at temperature T H Q L = magnitude of heat transfer between the cyclic device and the low temperature medium at temperature T L
Thermal efficiency (other expression) Also works with rate (dot)
EXAMPLE 6–1 Net Power Production Heat is transferred to a heat engine from a furnace at a rate of 80 MW. If the rate of waste heat rejection to a nearby river is 50 MW, determine the net power output and the thermal efficiency for this heat engine.
EXAMPLE 6–1 : Solution The furnace serves as the high-temperature reservoir for this heat engine and the river as the low- temperature reservoir.
EXAMPLE 6–2 Fuel Consumption of a Car A car engine with a power output of 65 hp has a thermal efficiency of 24 percent. Determine the fuel consumption rate of this car if the fuel has a heating value of 40,000 kJ/kg
EXAMPLE 6–2 : Solution 1 Hp = 746 W
The Second Law of Thermodynamics: Kelvin–Planck Statement Related to heat engines No heat engine can convert all the heat it receives to useful work. Kelvin–Planck statement of the second law of thermodynamics: It is impossible for any device that operates on a cycle to receive heat from a single reservoir and produce a net amount of work. An impossible Heat Engine
REFRIGERATORS Heat is transferred in the direction of decreasing temperature, that is, from high-temperature mediums to lowtemperature ones. This heat transfer process occurs in nature without requiring any devices. The reverse process, however, cannot occur by itself. The transfer of heat from a low-temperature medium to a high-temperature one requires special devices called refrigerators. Refrigeration cycle (vapor-compression refrigeration cycle) involves four main components: a compressor, a condenser, an expansion valve, and an evaporator.
Coefficient of Performance (COP R ) The efficiency of a refrigerator is measured by coefficient of performance (COP R ). In the US energy efficiency rating (EER). EER = COP R
HEAT PUMPS Device that transfers heat from a low-temperature medium to a high-temperature one is the heat pump.
Typical Rating Typical COP R : 2.6–3.0 for cutting and preparation rooms; 2.3–2.6 for meat, deli, dairy, and produce; 1.2–1.5 for frozen foods; 1.0–1.2 for ice cream units Typical EER of AC (COP AC ). Typical COP HP
EXAMPLE 6–3 Heat Rejection by a Refrigerator The food compartment of a refrigerator is maintained at 4°C by removing heat from it at a rate of 360 kJ/min. If the required power input to the refrigerator is 2 kW, determine (a) the COP R and (b) the rate of heat rejection to the room that houses the refrigerator.
EXAMPLE 6–3 : Solution (a) The coefficient of performance of the refrigerator is: (b) The rate of heat rejection is Q H : Notice that both the energy removed from the refrigerated space as heat and the energy supplied to the refrigerator as electrical work show up in the room air and become part of the internal energy of the air.
EXAMPLE 6–4 Heating a House by a Heat Pump A heat pump is used to meet the heating requirements of a house and maintain it at 20°C. On a day when the outdoor air temperature drops to 2°C, the house is estimated to lose heat at a rate of 80,000 kJ/h. If the heat pump under these conditions has a COP of 2.5, determine (a) the power consumed by the heat pump and (b) the rate at which heat is absorbed from the cold outdoor air.
EXAMPLE 6–3 : Solution (a) The power consumed by this heat pump: (b) The rate of heat transfer from the outdoor is Q L : Note that 48,000 of the 80,000 kJ/h heat is extracted from the cold outdoor air. Therefore, we are paying only for the 32,000-kJ/h energy as electrical work. If we use an electric resistance heater instead, we have to supply the entire 80,000 kJ/h as electric energy. The heating bill will be 2.5 times higher.
The Second Law of Thermodynamics: Clausius Statement Related to refrigerators or heat pumps It is impossible to construct a device that operates in a cycle and produces no effect other than the transfer of heat from a lower-temperature body to a higher- temperature body. An impossible Refrigerator
Kelvin–Planck vs. Clausius Statement Both are negative statements, and a negative statement cannot be proved. To date, no experiment has been conducted that contradicts the statement, and this is sufficient proof of its validity. Both statements are equivalent in their consequences, and either statement can be used as the expression of the second law of thermodynamics. Any device that violates the Kelvin–Planck statement also violates the Clausius statement, and vice versa.
AH THE CARNOT CYCLE
34 CARNOT ENGINE = IDEAL ENGINE In the early nineteenth century, the French scientist N.L. Sadi Carnot (1796 – 1832) studied in detail the process of transforming heat into mechanical energy. Goal to increase inefficiency. In 1824 Carnot invented, on paper, the Carnot engine. This is the ideal engine.
35 Reversible and Irreversible Processes The Carnot engine involves reversible processes. A reversible process is one carried out infinitely slowly, so that the process can be considered as a series of equilibrium states, and the whole process could be done in reverse with no change in magnitude of the work done or heat exchanged. Of course this cannot be done since it would take an infinite time. All real processes are irreversible: they cannot be done infinitely slowly, there can be turbulence in the gas, friction will be present, and so on.
36 Carnot's Engine The Carnot engine makes use of a reversible cycle. This cycle is called the Carnot cycle and the working substance is an ideal gas. Carnot heat-engine cycle is a totally reversible cycle, therefore, all the processes that comprise it can be reversed, in which case it becomes the Carnot refrigeration cycle.
37 Carnot Cycle
Thermodynamic Temperature Scale Lord Kelvin define a thermodynamic temperature scale as:
Carnot Efficiency and the Second Law Irreversible HE :Reversible HE = Carnot Efficiency = Max. Efficiency Carnots Theorem: All reversible engines operating between the same two constant temperatures T H and T L have the same efficiency. Any irreversible engine operating between the same two temperatures will have an efficiency less than this.
Carnot Efficiency Carnot efficiency is the best known reversible engine. This is the highest efficiency a heat engine operating between the two thermal energy reservoirs at temperatures T L and T H can have. Remind: T L and T H is absolute temperatures (K or R) 3 situation:
41 Example Steam engine efficiency. A steam engine operates between 500 o C and 270 o C. What is the maximum possible efficiency of this engine? SOLUTION: (do it yourself) max = 70,2 %
42 Example A phony claim? An engine manufacturer makes the following claims: The heat input per second of the engine is 9.0 kJ at 475 K. The heat output per second is 4.0 kJ at 325 K. Do you believe these claims? SOLUTION: NO (Proof yourself!!!)
Example A Carnot heat engine receives 500 kJ of heat per cycle from a high-temperature source at 652°C and rejects heat to a low-temperature sink at 30°C. Determine (a) the thermal efficiency of this Carnot engine, and (b) the amount of heat rejected to the sink per cycle.
Solution (a) Efficiency of Carnot heat engine is: (b) The amount of heat rejected Q L :
The Quality of Energy Consider the Carnot heat engine rejecting heat to a sink at 303 K. Now let us examine how the thermal efficiency varies with the source temperature (T H ). Conclusion: the higher the temperature, the higher the efficiency and, therefore, the higher the quality of the energy.
Lesson learned Work is a more valuable form of energy than heat since 100 percent of work can be converted to heat, but only a fraction of heat can be converted to work.
THE CARNOT REFRIGERATOR AND HEAT PUMP A refrigerator or a heat pump that operates on the reversed Carnot cycle is called a Carnot refrigerator, or a Carnot heat pump. The coefficient of performance (COP) of any refrigerator or heat pump, reversible or irreversible: The COP of reversible refrigerator or heat pump:
COP of Carnot R and HP 3 situations: Same situations can be made for heat pump by replacing COP R with COP HP.
EXAMPLE 6–6 A Questionable Claim An inventor claims to have developed a refrigerator that maintains the refrigerated space at 35°F while operating in a room where the temperature is 75°F and that has a COP of Is this claim reasonable?
EXAMPLE 6–6: Solution The performance of this refrigerator is: This is the highest COP a refrigerator. Since the COP claimed by the inventor is above this maximum value, the claim is false.
EXAMPLE 6–7 Carnot Heat Pump A heat pump is to be used to heat a house during the winter. The house is to be maintained at 21°C at all times. The house is estimated to be losing heat at a rate of 135,000 kJ/h when the outside temperature drops to 5°C. Determine the minimum power required to drive this heat pump.
EXAMPLE 6–7: Solution The heat pump must supply heat to the house at a rate of Q H 135,000 kJ/h or 37.5 kW. The COP of a reversible heat pump is: The required power input to this heat pump is