Refrigerators and Second Law of Thermodynamics
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Entropy in the Real World: Refrigerators
Chapter 20
Second Law of Thermodynamics
A
refrigerator
is a device that uses work to transfer energy from
a low-temperature reservoir to a high-temperature reservoir as the
device continuously repeats a series of thermodynamic processes.
In a household refrigerator, for example, work is done by an
electrical compressor to transfer energy from the food storage
compartment ( a low-temperature reservoir) to the room (a high-
temperature reservoir).
Air conditioners
and
heat pumps
are also refrigerators. The
differences are only in the nature of the high- and low-temperature
reservoirs.
For an air conditioner, the room is the low-temperature reservoir.
For a heat pump, the room is the high-temperature reservoir.
In an ideal refrigerator, all processes are reversible and no
wasteful energy transfers occur as a result of, say, friction and
turbulence.
Entropy in the Real World: Refrigerators
Chapter 20
Second Law of Thermodynamics
1.
Compressor: increasing pressure
increasing temperature,
enabling phase change from vapor to liquid
2.
Condenser: coils with tubing and many fins where condensation occurs
3.
Evaporator: coils with tubing and many fins where evaporation occurs
4.
Air handler: fan to circulate air
5.
Reversing valve: switch between heat pump and air conditioner
6.
Expansion valve: decreasing pressure
decreasing temperature,
enabling phase change from liquid to vapor
Entropy in the Real World: Refrigerators
Chapter 20
Second Law of Thermodynamics
The next figure shows the basic elements of an
ideal refrigerator.
Its operation is the reverse of how the Carnot
engine operates. All the direction of energy
transfers and work are reversed from those of a
Carnot engine.
We can call such an ideal refrigerator a
Carnot
refrigerator
.
The designer of a refrigerator would like to extract as much energy
|
Q
L
| as possible from the low-temperature reservoir (what we
want) for the least amount of work |
W
| (what we pay for).
A measure of the efficiency of a refrigerator expressed by
K
, called
the
coefficient of performance
:
Coefficient of Performance,
Any Refrigerator
Entropy in the Real World: Refrigerators
Chapter 20
Second Law of Thermodynamics
For a Carnot refrigerator, the first law of thermodynamics gives
|
W
| = |
Q
H
| – |
Q
L
|. Thus, the last equation then becomes
Coefficient of Performance,
Carnot Refrigerator
For household refrigerators,
K
≈ 5.
By examining the equation, we can find out that the value of
K
is
higher if the temperatures of the two reservoirs are closer to each
other.
Checkpoint
You wish to increase the coefficient of performance of an ideal
refrigerator. You can do so by
(a)
running the cold chamber at a
slightly higher temperature,
(b)
running the cold chamber at a
slightly lower temperature,
(c)
moving the unit to a slightly warmer
room, or
(d)
moving it to a slightly cooler room.
The magnitudes for the temperature changes are to be the same in
all four cases.
List the changes according to the resulting coefficients of
performance, greatest first.
(
a
)
,
(
d
)
,
(
c
)
,
a
n
d
(
b
)
Chapter 20
Second Law of Thermodynamics
Class Group Assignments
1.
The coefficient of performance of a household refrigerator is 5.2. The temperature
of the room where the refrigerator is located is 28°C. Determine the lowest
possible temperature inside the refrigerator?
(a)
–10.8°C
(b) –15.7°C
(c) –18.2°C
(d) –20.5°C
(e) –27.2°C
2.
The thermal reservoirs of a Carnot heat pump are at 27°C and 57°C. If the heat
pump is required to produce 100 kW heating effect, how much power does this
pump consume?
(a)
2.07 kW
(b) 9.1 kW
(c) 12.7 kW
(d) 15.3 kW
(e) 20.7 kW
3.
A vessel containing 5 kg of water at 10°C is put into a refrigerator. The 100 W
motor runs for 5 minutes to cool the liquid to the refrigerator’s low temperature,
0°C. What is the COP of the refrigerator?
(a)
5.7
(b) 4.6
(c) 6.9
(d) 7.2
(e) 3.6
Chapter 20
Second Law of Thermodynamics
Homework 10
1.
(20-39)
2.
(20-42)
Deadline:
Wednesday, 2 July 2014.
Validation test will be conducted in the beginning of the class.
Chapter 20
Second Law of Thermodynamics
Refrigerators are devices that transfer energy between low and high-temperature reservoirs using work. This process involves various thermodynamic cycles like the heat pump cycle and air conditioner cycle. The efficiency of refrigerators is described by the coefficient of performance, which is crucial for extracting energy efficiently. For Carnot refrigerators, the coefficient of performance is influenced by the temperature of the reservoirs.
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Thermal Physics Lecture 10 Dr.-Ing. Erwin Sitompul President University http://zitompul.wordpress.com 2 0 1 4 President University Erwin Sitompul Thermal Physics 10/1
Chapter 20 Second Law of Thermodynamics Entropy in the Real World: Refrigerators A refrigerator is a device that uses work to transfer energy from a low-temperature reservoir to a high-temperature reservoir as the device continuously repeats a series of thermodynamic processes. In a household refrigerator, for example, work is done by an electrical compressor to transfer energy from the food storage compartment ( a low-temperature reservoir) to the room (a high- temperature reservoir). Air conditioners and heat pumps are also refrigerators. The differences are only in the nature of the high- and low-temperature reservoirs. For an air conditioner, the room is the low-temperature reservoir. For a heat pump, the room is the high-temperature reservoir. In an ideal refrigerator, all processes are reversible and no wasteful energy transfers occur as a result of, say, friction and turbulence. President University Erwin Sitompul Thermal Physics 10/2
Chapter 20 Second Law of Thermodynamics Entropy in the Real World: Refrigerators 6 6 Heat Pump Cycle Air Conditioner Cycle 1. Compressor: increasing pressure increasing temperature, enabling phase change from vapor to liquid 2. Condenser: coils with tubing and many fins where condensation occurs 3. Evaporator: coils with tubing and many fins where evaporation occurs 4. Air handler: fan to circulate air 5. Reversing valve: switch between heat pump and air conditioner 6. Expansion valve: decreasing pressure decreasing temperature, enabling phase change from liquid to vapor President University Erwin Sitompul Thermal Physics 10/3
Chapter 20 Second Law of Thermodynamics Entropy in the Real World: Refrigerators The next figure shows the basic elements of an ideal refrigerator. Its operation is the reverse of how the Carnot engine operates. All the direction of energy transfers and work are reversed from those of a Carnot engine. We can call such an ideal refrigerator a Carnot refrigerator. The designer of a refrigerator would like to extract as much energy |QL| as possible from the low-temperature reservoir (what we want) for the least amount of work |W| (what we pay for). A measure of the efficiency of a refrigerator expressed by K, called the coefficient of performance: Q K W what we pay for what we want = = L Coefficient of Performance, Any Refrigerator President University Erwin Sitompul Thermal Physics 10/4
Chapter 20 Second Law of Thermodynamics Entropy in the Real World: Refrigerators For a Carnot refrigerator, the first law of thermodynamics gives |W| = |QH| |QL|. Thus, the last equation then becomes Q K Q Q T K T T = L H L Coefficient of Performance, Carnot Refrigerator = L H L For household refrigerators, K 5. By examining the equation, we can find out that the value of K is higher if the temperatures of the two reservoirs are closer to each other. President University Erwin Sitompul Thermal Physics 10/5
Chapter 20 Second Law of Thermodynamics Checkpoint You wish to increase the coefficient of performance of an ideal refrigerator. You can do so by (a) running the cold chamber at a slightly higher temperature, (b) running the cold chamber at a slightly lower temperature, (c) moving the unit to a slightly warmer room, or (d) moving it to a slightly cooler room. The magnitudes for the temperature changes are to be the same in all four cases. List the changes according to the resulting coefficients of performance, greatest first. (a), (d), (c), and (b) T = K L T T H L President University Erwin Sitompul Thermal Physics 10/6
Chapter 20 Second Law of Thermodynamics Class Group Assignments 1. The coefficient of performance of a household refrigerator is 5.2. The temperature of the room where the refrigerator is located is 28 C. Determine the lowest possible temperature inside the refrigerator? (a) 10.8 C (b) 15.7 C (c) 18.2 C (d) 20.5 C (e) 27.2 C 2. The thermal reservoirs of a Carnot heat pump are at 27 C and 57 C. If the heat pump is required to produce 100 kW heating effect, how much power does this pump consume? (a) 2.07 kW (b) 9.1 kW (c) 12.7 kW (d) 15.3 kW (e) 20.7 kW 3. A vessel containing 5 kg of water at 10 C is put into a refrigerator. The 100 W motor runs for 5 minutes to cool the liquid to the refrigerator s low temperature, 0 C. What is the COP of the refrigerator? (a) 5.7 (b) 4.6 (c) 6.9 (d) 7.2 (e) 3.6 President University Erwin Sitompul Thermal Physics 10/7
Chapter 20 Second Law of Thermodynamics Homework 10 1.(20-39) 2.(20-42) Deadline: Wednesday, 2 July 2014. Validation test will be conducted in the beginning of the class. President University Erwin Sitompul Thermal Physics 10/8
