week 9. refrigeration cycles i -...
TRANSCRIPT
Week 9. Refrigeration Cycles I
GENESYS Laboratory
Objectives
1. Introduce the concepts of refrigerators and heat pumps and the measure of their performance.
2. Analyze the ideal vapor-compression refrigeration cycle. 3. Analyze the actual vapor-compression refrigeration cycle. 4. Review the factors involved in selecting the right refrigerant for an
application. 5. Discuss the operation of refrigeration and heat pump systems. 6. Evaluate the performance of innovative vapor-compression
refrigeration system . 7. Analyze gas refrigeration systems. 8. Introduce the concepts of absorption-refrigeration systems. 9. Review the concepts of thermoelectric power generation and
refrigeration
GENESYS Laboratory
Refrigerators And Heat Pumps
• The transfer of heat from a low-temperature region to a high-temperature one
• The performance of refrigerators and heat pumps is expressed in terms of the
coefficient of performance (COP)
LR
net,in
HHP
net,in
HP R
Desired output Cooling effect
Required input Work input
Desired output Heating effect=
Required input Work input
1
QCOP
W
QCOP
W
COP COP
GENESYS Laboratory
The Reversed Carnot Cycle
Carnot refrigerator and T-s diagram of the reversed Carnot cycle
• Carnot Refrigerator
• Carnot Heat Pump
1
1COP CarnotR,
L
H
TT
H
L
TT
1
1COP CarnotHP,
The reversed Carnot cycle is not a suitable model for refrigeration cycles Process 1→2, 3→4 : achievable Process 2→3 the compression of a liquid-vapor mixture Process 4→1 the expansion of high- Moisture-content refrigerant in a turbine
GENESYS Laboratory
The Ideal Vapor-Compression Refrigeration Cycle
• Many of the impracticalities associated with the reversed Carnot cycle can be
eliminated by vaporizing the refrigerant completely before it is compressed and by
replacing the turbine with a throttling device, such as an expansion valve or
capillary
T-s diagram for the ideal vapor-compression refrigeration cycle
• Four processes: 1-2 Isentropic compression in a compressor 2-3 Constant-pressure heat rejection in a condenser 3-4 Throttling in an expansion device 4-1 Constant-pressure heat absorption in an evaporator
GENESYS Laboratory
The Ideal Vapor-Compression Refrigeration Cycle
• P-h diagram
-Process 3-4 is isenthalpic process (expansion valve)
-Processes 2-3 and 4-1: Q is determined as deviation between “h”s
-Process 1-2: W is determined as h2-h1
The P-h diagram of an ideal vapor-compression refrigeration cycle
12
32
innet,
HHP
12
41
innet,
LR
hh
hh
w
qCOP
hh
hh
w
qCOP
• The COPs of refrigerators and heat pumps operating on the vapor-compression refrigeration cycle can be expressed as
GENESYS Laboratory
Ex 1) The Ideal Vapor-Compression Refrigeration Cycle
GENESYS Laboratory
Ex 1-1) The Ideal Vapor-Compression Refrigeration Cycle
Consider an ideal refrigeration cycle that uses R-134a as the working fluid. The temperature of the refrigerant in the evaporator is -20oC, and in the condenser exit, it is 40oC. The refrigerant is circulated at the rate of 0.03 kg/s. Determine the COP and the capacity of the plant in rate of refrigeration.
GENESYS Laboratory
Actual Vapor-Compression Refrigeration Cycle
• An actual vapor-compression refrigeration cycle differs from the ideal one owing
to the irreversibilities (e.g. fluid friction causing pressure drops and heat transfer to
or from the surroundings) that occur in various components.
GENESYS Laboratory
• The compression process in the actual cycle is not isentropic • The entropy of the refrigerant may increase (process 1-2) or decrease (process 1-2’) due to cooling effect
• The refrigerant is subcooled somewhat before it enters the throttling valve and superheated before it enters the compressor
Ex 2) The Actual Vapor-Compression Refrigeration Cycle
GENESYS Laboratory
Ex 2-1) The Actual Vapor-Compression Refrigeration Cycle
A refrigeration cycle utilizes R-134a as the working fluid. The following are the properties at various points of the cycle designated in Figure. P1=125 kPa, T1=-10oC P2=1200 kPa, T2=100oC P3=1190 kPa, T3=80oC P4=1160 kPa, T4=45oC P5=1150 kPa, T5=40oC P6=P7=140 kPa, x6=x7 P8=130 kPa, T8=-20oC The heat transfer from R-134a during the compression process is 4 kJ/kg. Determine the COP of this cycle.
GENESYS Laboratory
Innovative Vapor-Compression Refrigeration Systems
• The ordinary vapor-compression refrigeration systems are simple, inexpensive,
reliable, and practically maintenance-free
• However, for large industrial applications efficiency, the major concern is not
simplicity.
• Modifications and refinements are necessary
- Cascade Refrigeration Systems
- Multistage Compression Refrigeration Systems
- Multipurpose Refrigeration Systems with a Single Compressor
- Liquefaction of Gases
GENESYS Laboratory
Cascade Refrigeration Systems
• Need to operate a large temperature range
-Way of dealing with a large pressure range in the cycle and a poor performance for
reciprocating compressor
• Solution
- Two or more refrigeration cycles that operate in series
-Refrigerants in both cycles can be the same or different, but a certain refrigerants
with more desirable characteristics can be used on each cycle
• Result
-The compressor work decreases and the
amount of heat absorbed from the refrige-
rated space increases
- The ratio of mass flow rates is
1256
41
innet,
LcascadeR,
85
323285
hhmhhm
hhm
W
QCOP
hh
hh
m
mhhmhhm
BA
B
B
ABA
GENESYS Laboratory