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3/30/2017
1
FET 411, Refrigeration and Air
Conditioning Engineering
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Course outline
• Chapter 1: Introduction to Refrigeration
• Chapter 2: Refrigeration cycle
• Chapter 3: Equipments of Refrigerator
• Chapter 4: Properties of Refrigerant
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Reference books
• Refrigeration and Air Conditioning – P. L. Ballaney
• A text book of Refrigeration and Air Conditioning – R.S.
Khurmi
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Chapter 1: Introduction to Refrigeration
• Refrigeration may be defined as the process of removing heat
or heat energy from a body, that is below the temperature of
its surroundings.
Refrigeration
Natural
Mechanical
Compression
Absorption: Ammonia and
water vapor
Steam jetMd Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
3/30/2017
2
Objectives
• To understand why the storage life of foods and agricultural
products can be extended by refrigeration
• To learn the adverse effects of low temperature for certain
commodities
• To refresh our knowledge about thermodynamics, in particular the
first law of thermodynamics, the phase diagram and the Mollier
diagram
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Purpose of refrigeration of foods
- reduces postharvest losses
- preserves foods
- makes it possible to provide safe, wholesome food all consumers
have the right to expect
- by refrigerated transport, allows countries to export perishable
produce
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
How does it work?
Fig. Gas production rate as a function of developmental stage
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
3/30/2017
3
Q10 (reduction in reaction rate if temperature decreases by 10°C) typically
2.5 for biochemical reactions
• Respiration
• Texture change
• Microbial growth
Example
- Predictive microbiology: prediction of microbial growth/inactivation in
various conditions of temperature, gas concentration, salt etc.
- E.g. Pathogen Modeling Program
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Negative effects of refrigeration: Chilling injury
- Variety of symptoms: lesions, brown heart in pineaple, mealiness in
tomato, gery discoloration in banana
- Most tropical fruits are affected
- Typically below 12°C, depending on cultivar
- Believed to be caused by imbalance between saturated and unsaturated
lipids
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
3/30/2017
4
Importance of refrigeration
- Number of farmers has gradually increased: <5% of world population
- Cold chains are vital to ensure safety, quality and commercial value of perishable
foodstuffs
- 75% of foods are processed, the majority involves one or more refrigeration steps
- Foods or ingredients are transported 2.5 times
- Approximately 70% of foods in developed countries are chilled or frozen when
produced, and 50% of all foods sold require refrigerated display at retailer level
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
A few numbers
- Annual purchase of chilled and quick-frozen foods is around 1200 billion
USD
- Refrigeration generates jobs: 1 out of 1000 jobs in industrialized
countries are in the equipment manufacturing field
- 300000 jobs in the USA and 70000 in Europe in the installation and
sectors
- Annual investment in refrigerating equipment totals 170 billion USD
- More than 1 billion domestic refrigerators/freezers in the world
- 300 m3 of cold storage worldwide
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Simple cooling systems
• Pot – in – Pot (M. Bah Abba)
- Two ceramic pots
- Smallest pot inside largest pot
- Wet soil in between
- Cooling via evaporation: latent heat (enthalpy removed from pot
- Rolex award
- Simple design, local manufacturing possible
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
3/30/2017
5
Thermodynamics of phase change
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Temperature Vs Total Heat
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
State diagram
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Units of Refrigeration
• Unit of refrigeration: Tonne of refrigeration (TR)
• A tonne of refrigeration is defined as the amount of refrigeration effect
produced by the uniform melting of one tonne (1000kg) of ice from and at
0 oC in 24 hrs.
• Latent heat of ice is 335 KJ/Kg, hence,
• 1TR= 1000 Kg * 335 KJ/Kg in 24 hrs
= (1000*335)/ (24*60)
= 232.6 KJ/min (in actual 210 KJ/min or 3.5 KW)
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
3/30/2017
6
Coefficient of performance
• COP = Amount of heat extracted in the refrigerator (Q)/ amount of
work done (W)
= Q/W
• It is reciprocal of the efficiency of a heat engine
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Difference between Heat engine, Refrigerator and heat pump
COP (E) = Work done
(W)/ Heat supplied (Q2)
=(Q2 – Q1)/ Q2
COP (R) = Heat taken
(Q2)/ Work done (W)
=Q1/ (Q2- Q1)
COP (P) = Heat delivered
(Q1)/ Work done (W)
= Q1/ (Q2- Q1)
= COP (R) + 1
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Simple vapor compression refrigeration system
• It is named as vapor compression, due to low pressure vapor
refrigerant from the evaporator is changed to high pressure
vapor in the compressor.
• Refrigerant: NH3, CO2, SO2
• Advantage: small, less running cost, can be run over large
range of temperatures, COP is high.
• Disadvantage: Initial cost high, leakage problem
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
3/30/2017
7
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Mechanism of a simple vapor compression refrigeration
system
1. Compressor: Low pressure, temp vapor refrigerant from evaporator drawn into
compressor at high temp through suction valve. The highly pressed and temp
vapor refrigerant is discharged into the condenser through discharge valve.
2. Condenser (cooler): Refrigerant cooled and condensed here. At this stage,
refrigerant gives up its latent heat to the surroundings condensing medium
(air/water).
3. Receiver: the condensed refrigerant stored here in a vessel.
4. Expansion valve (refrigerant control valve): allow the liquid high pressure
refrigerant in a controlled reducing rate. Some portion of refrigerant evaporates
here but greater are evaporate in evaporator.
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
5. Evaporator: The liquid-vapor refrigerant are passed through evaporator
(consists of coils of pipe) at low pressure and temperature. Here, the
liquid refrigerant absorbs its latent heatof vaporisation from the medium
(air, water or brine) which is to be cooled.
High pressure side: discharge line, condenser, receiver and expansion valve.
Low pressure side: evaporator, piping from expansion valve to evaporator and
the suction line.
Check the link for more: https://www.mobileair.com/refrigeration-cycle
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
3/30/2017
8
Pressure- enthalpy diagram
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
• Red line: temperature
• Green line: constant volume curve
• Black line: quality curves or mass fraction of vapor
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
3/30/2017
9
• COP = Refrigeration effect/ Work done
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Factors influencing COP
1. There is no pressure loss in condenser, evaporator, connecting pipes and
compressor valves.
2. There is no heat transfer form or to the system at any point except the
condenser and evaporator
3. Compression is isentropic.
4. Transmission efficiency is from motor to compressor is 100%
5. Condenser temperature increase then COP is decrease due to
decreasing refrigeration effect.
6. Subcooling
7. Superheating
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Actual refrigeration cycle
1. The liquid refrigerant in the condenser may be undercooled,
i.e. cooled below the condensing temperature before
passing through the expansion valve. This can be obtained
by large quantities of circulating cooling water which should
be at a temperature much lower than the condensing
temperatures.
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
2. Normally the gas leaves the evaporator in superheated condition
before it enters the compressor. This superheating may occur in
the evaporator pipes leaving the evaporator but still in the cooled
space. Thus the refrigerating effect will increase per kg of
refrigerant flow. This superheating may occur in the pipes
connecting the evaporator delivery and the compressor suction, in
spite of these pipes being insulated. Thus this is a loss or an
additional load on the compressor and condenser without any
useful cooling effect obtained. Thus these pipes should be
properly insulated.
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
3/30/2017
10
3) Compression has been assumed isentropic, but in actual practice it
may be very complex. The cylinder wall may be stabilize at a
temperature between the cool suction gas and hot discharge gas.
Thus during the first part of compression heat may flow from the
walls to the gas and in the later part of the stroke the reversal in the
direction of flow of heat may take place.
4) The refrigerant has to flow through pipes in the evaporator,
condenser and other connecting pipes. In actual practice due to
frictional resistance to flow, there is pressure fall in the connecting
pipes.
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Effect of Subcooling
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Effect of Superheating
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
A-B: isentropic compression
B-C: removal of superheat
C-D: removal of heat of condensation (isothermal)
D-E: expansion in expansion valve (isenthalpyl)
E-A: evaporation at the evaporator (isothermal)
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
3/30/2017
11
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Pressure Enthalpy charts
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
3/30/2017
12
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
3/30/2017
13
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
3/30/2017
14
• Cooling load
o Rate of heat energy removal
o “Ton of refrigeration”: latent heat of fusion of 1 ton of ice per day = 3.52
kW
• Heat to be removed
o Heat of respiration
o Losses through ceiling, floor and wall
o Heat production of fans, lights, fork lifts, personnel
• Condenser
o Heat rejected to environment:
3 1( )cq m H H 
1
2
3
H Enthalphy of refrigerant at exit from
the condonsor (kJ/kg)
H ethalphy of refrigerant at the beginning
of compression of stroke (kJ/kg refrigerant)
H ethalphy of refrigerant at the


 end
of compression of stroke (kJ/kg refrigerant)
m refrigerant mass flow rate (kg/s)Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Mathematical expressions: Design and
analysis
• Evaporator
• Compressor
• Coefficient of performance
o Indicator of efficiency of system
o Ratio of useful effect to the work expended
o Coefficient Of Performance: heat absorbed by refrigerant / energy supplied
to compressor
o Refrigerant flow rate (q is heat to be removed)
2 1( )eq m H H 
3 2( )wq m H H 
2 1
3 2
H H
COP
H H


 2 1
q
m
H H



c
e
w
q rate of heat exchanged in the condensor (kW)
q rate of heat exchanged from the evaporator (kW)
q rate of work done on the refrigerant (kW)



Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Charging of refrigeration system
• After completely assemble of refrigeration system, the whole system is
tested for leaks, dried and evacuation, it is ready for charging.
• The refrigerant to be used is stored in liquid form in suitable containers.
• The usual practice is to feed refrigerant vapor from the top of the
container into the suction line of the system with the compressor running
and condenser in operation.
• The rate of removal of refrigerant from container, is accelerated by
immersing in hot water. It is important to supply the correct amount of
refrigerant into the system.
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Common troubles in refrigeration system
• A large portion of service trouble with refrigeration system is
caused by MOISTURE.
• One small drop of liquid water can stop the circulation of
refrigerant by freezing in the expansion device.
• Other troubles such as corrosion, copper plating and
chemical damage to insulation may result if moisture is
present in the system.
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
3/30/2017
15
How water may appear in refrigeration system
1. Incomplete drying of the equipment before charging,
2. Low sides leaks admitting air which contains moisture,
3. Leakage in water-cooled condenser,
4. Water formation through oxidation of certain hydrocarbons in
the oil
5. Water dissolved in either oil or liquid refrigerant when it is
placed in the system and
6. Decomposition of the motor insulation in hermetically sealed
units.
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Remedies of moisture removal
By using dessicant (drying agent) or absorbent and
chemical driers to remove water from the
refrigeration system.
1. Absorbents: Granular aluminium oxide (activated
alumina), silicon dioxide (silica gel),
2. Chemical driers: anhydrous calcium sulfate (drierite),
calcium oxide or quiklime and calcium chloride.
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Troubles with non-condensable gases
• They are also service troubles with refrigerating system. They increase
operating pressures and temperatures and decrease efficiency. They
present in refrigeration system from one or more of the following sources:
1. Incomplete removal of the gas used for pressure testing the system prior
to charging,
2. Formation of non-condensable gas by chemical reactions within the
system.
3. Air and othe rnon-condensable gases dissolved in the refrigerant when
charged and
4. Leaks in the piping.
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Remedies for non-condensable gases
• Small unit: it is removed by wasting the charge, evacuating
the system and recharging with fresh refrigerant.
• Large unit: it can be removed from the top of the
condenser and from the top of the evaporator with an
accompanying loss of only a small portion of the refrigerant
charge. The process of removing non-condensable gases
from a refrigerating system is called purging.
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
3/30/2017
16
Tests for leakage of the refrigerant
1. Leakage of SO2: detected by the white smoke which
appears if a swab soaked with a 25% solution of aqueous
NH3 is brought near it.
2. Leakage of NH3: may be detected with burning sulfur
candle.
3. Leakage of freons (halogenated hydrocarbons): may be
detected by the use of halde torch. (The halide torch
burns alcohol and the flame turns green in the presence
of freon vapours).
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Methods of defrosting
• In many compression refrigeration systems the evaporator is a direct expansion
coil used to cool and dehumidifying the air passes over it. If the condition of
operation require metal surface below 32 oF, frost will collect on the tubes and
fins and periodic defrosting is essential.
• The methods of collecting frosts are
i. Interrupted service
ii. Water spray
iii. Hot gas and hot oil
iv. Electric resistance heater adjacent coil or arrangement for heating coil
by passing low voltage current through the metal.
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST
Control compression refrigeration system
• Small systems (household refrigerator and home AC): the compressor is
stopped when the cooling thermostat has been satisfied and it is started
again when further refrigeration is needed.
• Large systems: The centrifugal compressor’s capacity may be varied to
match a changing load by
i. Varying the speed
ii. Adjusting vanes all the inlet to the impellers
iii. Regulators which throttle the suction gas so as to keep the evaporator
pressure constant and control the volume
iv. Varying condenser pressure.
Md Rahmatuzzaman Rana
AssistantProfessor, Dept of FET, SUST

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Refrigeration and Air Conditioning Engineering (Lecture 01)

  • 1. 3/30/2017 1 FET 411, Refrigeration and Air Conditioning Engineering Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Course outline • Chapter 1: Introduction to Refrigeration • Chapter 2: Refrigeration cycle • Chapter 3: Equipments of Refrigerator • Chapter 4: Properties of Refrigerant Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Reference books • Refrigeration and Air Conditioning – P. L. Ballaney • A text book of Refrigeration and Air Conditioning – R.S. Khurmi Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Chapter 1: Introduction to Refrigeration • Refrigeration may be defined as the process of removing heat or heat energy from a body, that is below the temperature of its surroundings. Refrigeration Natural Mechanical Compression Absorption: Ammonia and water vapor Steam jetMd Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST
  • 2. 3/30/2017 2 Objectives • To understand why the storage life of foods and agricultural products can be extended by refrigeration • To learn the adverse effects of low temperature for certain commodities • To refresh our knowledge about thermodynamics, in particular the first law of thermodynamics, the phase diagram and the Mollier diagram Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Purpose of refrigeration of foods - reduces postharvest losses - preserves foods - makes it possible to provide safe, wholesome food all consumers have the right to expect - by refrigerated transport, allows countries to export perishable produce Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST How does it work? Fig. Gas production rate as a function of developmental stage Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST
  • 3. 3/30/2017 3 Q10 (reduction in reaction rate if temperature decreases by 10°C) typically 2.5 for biochemical reactions • Respiration • Texture change • Microbial growth Example - Predictive microbiology: prediction of microbial growth/inactivation in various conditions of temperature, gas concentration, salt etc. - E.g. Pathogen Modeling Program Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Negative effects of refrigeration: Chilling injury - Variety of symptoms: lesions, brown heart in pineaple, mealiness in tomato, gery discoloration in banana - Most tropical fruits are affected - Typically below 12°C, depending on cultivar - Believed to be caused by imbalance between saturated and unsaturated lipids Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST
  • 4. 3/30/2017 4 Importance of refrigeration - Number of farmers has gradually increased: <5% of world population - Cold chains are vital to ensure safety, quality and commercial value of perishable foodstuffs - 75% of foods are processed, the majority involves one or more refrigeration steps - Foods or ingredients are transported 2.5 times - Approximately 70% of foods in developed countries are chilled or frozen when produced, and 50% of all foods sold require refrigerated display at retailer level Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST A few numbers - Annual purchase of chilled and quick-frozen foods is around 1200 billion USD - Refrigeration generates jobs: 1 out of 1000 jobs in industrialized countries are in the equipment manufacturing field - 300000 jobs in the USA and 70000 in Europe in the installation and sectors - Annual investment in refrigerating equipment totals 170 billion USD - More than 1 billion domestic refrigerators/freezers in the world - 300 m3 of cold storage worldwide Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Simple cooling systems • Pot – in – Pot (M. Bah Abba) - Two ceramic pots - Smallest pot inside largest pot - Wet soil in between - Cooling via evaporation: latent heat (enthalpy removed from pot - Rolex award - Simple design, local manufacturing possible Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST
  • 5. 3/30/2017 5 Thermodynamics of phase change Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Temperature Vs Total Heat Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST State diagram Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Units of Refrigeration • Unit of refrigeration: Tonne of refrigeration (TR) • A tonne of refrigeration is defined as the amount of refrigeration effect produced by the uniform melting of one tonne (1000kg) of ice from and at 0 oC in 24 hrs. • Latent heat of ice is 335 KJ/Kg, hence, • 1TR= 1000 Kg * 335 KJ/Kg in 24 hrs = (1000*335)/ (24*60) = 232.6 KJ/min (in actual 210 KJ/min or 3.5 KW) Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST
  • 6. 3/30/2017 6 Coefficient of performance • COP = Amount of heat extracted in the refrigerator (Q)/ amount of work done (W) = Q/W • It is reciprocal of the efficiency of a heat engine Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Difference between Heat engine, Refrigerator and heat pump COP (E) = Work done (W)/ Heat supplied (Q2) =(Q2 – Q1)/ Q2 COP (R) = Heat taken (Q2)/ Work done (W) =Q1/ (Q2- Q1) COP (P) = Heat delivered (Q1)/ Work done (W) = Q1/ (Q2- Q1) = COP (R) + 1 Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Simple vapor compression refrigeration system • It is named as vapor compression, due to low pressure vapor refrigerant from the evaporator is changed to high pressure vapor in the compressor. • Refrigerant: NH3, CO2, SO2 • Advantage: small, less running cost, can be run over large range of temperatures, COP is high. • Disadvantage: Initial cost high, leakage problem Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST
  • 7. 3/30/2017 7 Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Mechanism of a simple vapor compression refrigeration system 1. Compressor: Low pressure, temp vapor refrigerant from evaporator drawn into compressor at high temp through suction valve. The highly pressed and temp vapor refrigerant is discharged into the condenser through discharge valve. 2. Condenser (cooler): Refrigerant cooled and condensed here. At this stage, refrigerant gives up its latent heat to the surroundings condensing medium (air/water). 3. Receiver: the condensed refrigerant stored here in a vessel. 4. Expansion valve (refrigerant control valve): allow the liquid high pressure refrigerant in a controlled reducing rate. Some portion of refrigerant evaporates here but greater are evaporate in evaporator. Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST 5. Evaporator: The liquid-vapor refrigerant are passed through evaporator (consists of coils of pipe) at low pressure and temperature. Here, the liquid refrigerant absorbs its latent heatof vaporisation from the medium (air, water or brine) which is to be cooled. High pressure side: discharge line, condenser, receiver and expansion valve. Low pressure side: evaporator, piping from expansion valve to evaporator and the suction line. Check the link for more: https://www.mobileair.com/refrigeration-cycle Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST
  • 8. 3/30/2017 8 Pressure- enthalpy diagram Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST • Red line: temperature • Green line: constant volume curve • Black line: quality curves or mass fraction of vapor Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST
  • 9. 3/30/2017 9 • COP = Refrigeration effect/ Work done Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Factors influencing COP 1. There is no pressure loss in condenser, evaporator, connecting pipes and compressor valves. 2. There is no heat transfer form or to the system at any point except the condenser and evaporator 3. Compression is isentropic. 4. Transmission efficiency is from motor to compressor is 100% 5. Condenser temperature increase then COP is decrease due to decreasing refrigeration effect. 6. Subcooling 7. Superheating Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Actual refrigeration cycle 1. The liquid refrigerant in the condenser may be undercooled, i.e. cooled below the condensing temperature before passing through the expansion valve. This can be obtained by large quantities of circulating cooling water which should be at a temperature much lower than the condensing temperatures. Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST 2. Normally the gas leaves the evaporator in superheated condition before it enters the compressor. This superheating may occur in the evaporator pipes leaving the evaporator but still in the cooled space. Thus the refrigerating effect will increase per kg of refrigerant flow. This superheating may occur in the pipes connecting the evaporator delivery and the compressor suction, in spite of these pipes being insulated. Thus this is a loss or an additional load on the compressor and condenser without any useful cooling effect obtained. Thus these pipes should be properly insulated. Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST
  • 10. 3/30/2017 10 3) Compression has been assumed isentropic, but in actual practice it may be very complex. The cylinder wall may be stabilize at a temperature between the cool suction gas and hot discharge gas. Thus during the first part of compression heat may flow from the walls to the gas and in the later part of the stroke the reversal in the direction of flow of heat may take place. 4) The refrigerant has to flow through pipes in the evaporator, condenser and other connecting pipes. In actual practice due to frictional resistance to flow, there is pressure fall in the connecting pipes. Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Effect of Subcooling Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Effect of Superheating Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST A-B: isentropic compression B-C: removal of superheat C-D: removal of heat of condensation (isothermal) D-E: expansion in expansion valve (isenthalpyl) E-A: evaporation at the evaporator (isothermal) Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST
  • 11. 3/30/2017 11 Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Pressure Enthalpy charts Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST
  • 12. 3/30/2017 12 Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST
  • 13. 3/30/2017 13 Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST
  • 14. 3/30/2017 14 • Cooling load o Rate of heat energy removal o “Ton of refrigeration”: latent heat of fusion of 1 ton of ice per day = 3.52 kW • Heat to be removed o Heat of respiration o Losses through ceiling, floor and wall o Heat production of fans, lights, fork lifts, personnel • Condenser o Heat rejected to environment: 3 1( )cq m H H  1 2 3 H Enthalphy of refrigerant at exit from the condonsor (kJ/kg) H ethalphy of refrigerant at the beginning of compression of stroke (kJ/kg refrigerant) H ethalphy of refrigerant at the    end of compression of stroke (kJ/kg refrigerant) m refrigerant mass flow rate (kg/s)Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Mathematical expressions: Design and analysis • Evaporator • Compressor • Coefficient of performance o Indicator of efficiency of system o Ratio of useful effect to the work expended o Coefficient Of Performance: heat absorbed by refrigerant / energy supplied to compressor o Refrigerant flow rate (q is heat to be removed) 2 1( )eq m H H  3 2( )wq m H H  2 1 3 2 H H COP H H    2 1 q m H H    c e w q rate of heat exchanged in the condensor (kW) q rate of heat exchanged from the evaporator (kW) q rate of work done on the refrigerant (kW)    Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Charging of refrigeration system • After completely assemble of refrigeration system, the whole system is tested for leaks, dried and evacuation, it is ready for charging. • The refrigerant to be used is stored in liquid form in suitable containers. • The usual practice is to feed refrigerant vapor from the top of the container into the suction line of the system with the compressor running and condenser in operation. • The rate of removal of refrigerant from container, is accelerated by immersing in hot water. It is important to supply the correct amount of refrigerant into the system. Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Common troubles in refrigeration system • A large portion of service trouble with refrigeration system is caused by MOISTURE. • One small drop of liquid water can stop the circulation of refrigerant by freezing in the expansion device. • Other troubles such as corrosion, copper plating and chemical damage to insulation may result if moisture is present in the system. Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST
  • 15. 3/30/2017 15 How water may appear in refrigeration system 1. Incomplete drying of the equipment before charging, 2. Low sides leaks admitting air which contains moisture, 3. Leakage in water-cooled condenser, 4. Water formation through oxidation of certain hydrocarbons in the oil 5. Water dissolved in either oil or liquid refrigerant when it is placed in the system and 6. Decomposition of the motor insulation in hermetically sealed units. Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Remedies of moisture removal By using dessicant (drying agent) or absorbent and chemical driers to remove water from the refrigeration system. 1. Absorbents: Granular aluminium oxide (activated alumina), silicon dioxide (silica gel), 2. Chemical driers: anhydrous calcium sulfate (drierite), calcium oxide or quiklime and calcium chloride. Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Troubles with non-condensable gases • They are also service troubles with refrigerating system. They increase operating pressures and temperatures and decrease efficiency. They present in refrigeration system from one or more of the following sources: 1. Incomplete removal of the gas used for pressure testing the system prior to charging, 2. Formation of non-condensable gas by chemical reactions within the system. 3. Air and othe rnon-condensable gases dissolved in the refrigerant when charged and 4. Leaks in the piping. Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Remedies for non-condensable gases • Small unit: it is removed by wasting the charge, evacuating the system and recharging with fresh refrigerant. • Large unit: it can be removed from the top of the condenser and from the top of the evaporator with an accompanying loss of only a small portion of the refrigerant charge. The process of removing non-condensable gases from a refrigerating system is called purging. Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST
  • 16. 3/30/2017 16 Tests for leakage of the refrigerant 1. Leakage of SO2: detected by the white smoke which appears if a swab soaked with a 25% solution of aqueous NH3 is brought near it. 2. Leakage of NH3: may be detected with burning sulfur candle. 3. Leakage of freons (halogenated hydrocarbons): may be detected by the use of halde torch. (The halide torch burns alcohol and the flame turns green in the presence of freon vapours). Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Methods of defrosting • In many compression refrigeration systems the evaporator is a direct expansion coil used to cool and dehumidifying the air passes over it. If the condition of operation require metal surface below 32 oF, frost will collect on the tubes and fins and periodic defrosting is essential. • The methods of collecting frosts are i. Interrupted service ii. Water spray iii. Hot gas and hot oil iv. Electric resistance heater adjacent coil or arrangement for heating coil by passing low voltage current through the metal. Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST Control compression refrigeration system • Small systems (household refrigerator and home AC): the compressor is stopped when the cooling thermostat has been satisfied and it is started again when further refrigeration is needed. • Large systems: The centrifugal compressor’s capacity may be varied to match a changing load by i. Varying the speed ii. Adjusting vanes all the inlet to the impellers iii. Regulators which throttle the suction gas so as to keep the evaporator pressure constant and control the volume iv. Varying condenser pressure. Md Rahmatuzzaman Rana AssistantProfessor, Dept of FET, SUST