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MODELLING AND SIMULATION OF
NATURAL REFRIGERATION SYSTEMS
EXTERNAL GUIDE:
Dr.SUNIL SHAH
(CEO Modelicon InfoTech LLP)
EVAN AALEX 1MS20CH016
NEHA S PATWARDHAN 1MS20CH024
SARAH FATIMA 1MS20CH030
VISHWANATH SABARAD 1MS20CH043
DEPARTMENT OF
CHEMICAL ENGINEERING
PROJECT GUIDE:
Dr.BRIJESH
TABLE OF CONTENTS
1. Scope
2. Objectives
3. Introduction
4. Vapour Compression Refrigeration Cycle
5. Modelling and Simulation
6. Results and Discussions
• COP and Flow rate trends
• Comparison based on COP
• Sensitivity analysis
• Optimization
7. Conclusion
Comparison of refrigerants based on factors
such as environmental impact, safety
considerations, application specificity, cost and
energy consumption helps in selection of the
best suited model for the respective application.
SIMULATION
• To optimize the design and maximize the system
efficiency by minimizing energy consumption
and operating cost.
• To scale up the process.
The global green refrigerants market was valued at
US$ 18.8 billion in 2022 and is expected to reach US$
32.1 billion by 2030.
FUTURE OF REFRIGERANTS
• Predict refrigeration system performance with
respect to parameters such as cooling capacity,
COP, temperature etc.
• Process optimization by adjusting parameters such
as flow rate, pressure ratio, temperature etc.
MODELLING
COMPARISON
SCOPE
OBJECTIVES
 Model and simulate a simple refrigeration loop for each of the four fluids –
carbon dioxide, ammonia, isobutane, and 2,3,3,3-tetrafluoropropene (R1234yf)
using Aspen HYSYS.
 Analyse the refrigeration loops over a range of operating conditions and conduct
sensitivity analysis.
 Compare these models on the basis of their performance.
 Optimize each refrigeration loop to maximize COP
INTRODUCTION
• Refrigeration technology plays an
important role in various industries
• 15–20% of the world’s electricity is
used by refrigeration (Yatangababa et al., 2015)
• Most synthetic refrigerants, released
into the atmosphere cause depletion of
ozone layer and global warming.
• Natural refrigerants have low or no
GWP and ODP. (Cavallini 2020; Abas et al.,2018)
REFIGERANTS AND THEIR PROPERTIES
Refrigerant R717 R744 R600a R1234yf
Chemical Formula NH3 CO2 CH(CH3)2CH3 CF3CF=CH2
GWP <1 1 4 <1
ODP 0 0 0 0
Critical Pressure (MPa) 11.33 7.38 3.64 3.4
Critical Temperature (oC) 132.2 31.1 134.7 94.7
Normal Boiling Point (oC) -33 -78.4 -11.7 -29.54
Specific Heat capacity
(kJ/kg-K)
4.7 0.63 2.4 1.39
Latent Heat (kJ/kg) 1370 571.0 345.83 180.25
ASHRAE safety group A1 A1 A3 A2L
ASHRAE flammability No No Yes (high) Yes (mild)
ASHRAE toxicity Yes No No No
• Ammonia – R717
• Carbon Dioxide – R744
• Isobutane – R600a
• 2,3,3,3-Tetrafluoropropene
– R1234yf
(Kyriakides et al.,2020)
VAPOUR COMPRESSION
REFRIGERATION SYSTEMS (VCRS)
VCRS mainly consists of – Chilled fluid Fluid
EVAPORATOR
CONDENSER
COMPRESSOR
VALVE
Cooling fluid
Evaporator: Heat is absorbed from the medium to
be cooled. Refrigerant evaporates.
Compressor: Refrigerant is compressed to high
temperature and pressure. Compressor circulates
the refrigerant.
Condenser: Refrigerant gives up heat and is
condensed to a liquid.
Expansion valve: High-pressure refrigerant expands
to low temperature and pressure.
Specifications Value Unit
Chiller Capacity 200 kW
Chiller water inlet Temperature 12 ℃
Chiller water outlet Temperature 7 ℃
Evaporator Superheat 0, 1, 2 ℃
Cooling water inlet Temperature (Condenser) 24 ℃
Cooling water outlet Temperature (Condenser) 28 ℃
Table 1: Process conditions of the
simulation
Process flow sheet
STEADY STATE MODELLING
Equipment Parameter Equation
Evaporator Heat Balance (kW) Q=m Cp ∆T
Compressor
Work done (kW)
Volumetric Capacity (m3/hr)
𝑊 = 𝑧𝑅𝑇
𝛾
𝛾 − 1
[(
𝑃𝑑
𝑃𝑠
)
𝛾−1
𝛾 − 1] × 𝑚
𝑉 =
𝑚
𝜌
Condenser Heat Balance (kW) Q=m Cp ∆T
Expansion
Valve
Pressure Drop (kPa) Δ𝑃 =
Δ𝐻
𝜌. 𝑔. 𝜂
Overall
System
Coefficient of Performance
(COP)
Carnot COP
𝐶𝑂𝑃 =
𝐸𝑣𝑎𝑝𝑜𝑟𝑎𝑡𝑜𝑟 𝐷𝑢𝑡𝑦
𝐶𝑜𝑚𝑝𝑟𝑒𝑠𝑠𝑜𝑟 𝐷𝑢𝑡𝑦
𝐶𝑂𝑃 =
𝑇𝑒
𝑇𝑐 − 𝑇𝑒
Q – heat rate (kW)
m – mass flowrate (kg/h)
Cp – Constant pressure specific heat
capacity
T – absolute temperature (K)
z – compressibility factor
R – universal gas constant (J/mol-K)
Pd – Discharge pressure
Ps – suction pressure
𝜌 – density of fluid (kg/m3)
𝛾 – adiabatic index
𝜂 – adiabatic efficiency
Te − Evaporator temperature (K)
Tc – condenser temperature (K)
SIMULATION
1. SETTING THE PROPERTIES
2. SIMULATION ENVIRONMENT
• Four components
• Peng-Robinson fluid package
Heat exchangers
• Tube side – water, Shell side – refrigerant
• Pressure drop
• Chilling water flow rate = 33350 kg/hr
• Inlet and outlet temperatures
Compressor
• Efficiency = 75%
• Pressure ratio = 3
RESULTS AND DISCUSSIONS
0
2
4
6
8
10
-15 -10 -5 0 5 10
COP
Evaporation Temperature (°C)
Carbon dioxide
Tc = 30 ℃
Tc = 25 ℃
Tc = 20 ℃
0
1
2
3
4
5
6
7
8
-40 -30 -20 -10 0 10
COP
Evaporation temperature (℃)
Ammonia
Tc = 30℃
Tc = 35℃
Tc = 40℃
Tc = 45℃
0
1
2
3
4
5
6
-7.5 -5 -2.5 0 2.5 5 7.5
COP
Evaporation Temperature (℃)
R1234yf
Tc = 40 ℃
Tc = 45 ℃
Tc = 50 ℃
Tc = 55 ℃
0
1
2
3
4
5
6
7
8
-40 -30 -20 -10 0 10
COP Evaporation temperature (C)
Iso-butane Tc = 30 ℃
Tc = 35 ℃
Tc = 40 ℃
Tc = 45 ℃
COP vs Evaporator Temperature
Mass flow rate vs Evaporator Temperature
0.00
5000.00
10000.00
15000.00
20000.00
25000.00
-40 -30 -20 -10 0 10
Mass
Flowrate
(kg/hr)
Evaporator Temperature (⁰C)
R-1234yf
Tc = 30 ⁰C
Tc = 35 ⁰C
Tc = 40 ⁰C
Tc = 45 ⁰C
0
2000
4000
6000
8000
10000
12000
14000
16000
0 10 20 30 40
Flow
rate
(kg/hr)
Evaporator duty (kJ/hr)
x 100000
Isobutane
0
20000
40000
60000
80000
100000
0 300 600 900 1200
Flowrate
(kg/hr)
Evaporator Duty (kJ/hr) x 100000
Ammonia
R1234yf Carbon Dioxide
Mass flowrate vs Evaporator Duty
COMPARISON
Ammonia – Better
thermodynamic properties
Iso-butane – hydrocarbon
R1234yf – hydrocarbon
Carbon dioxide – subcritical state
Ammonia
Carbon dioxide
Iso-butane
R1234yf
OPTIMIZATION
𝐶𝑂𝑃 =
𝐸𝑣𝑎𝑝𝑜𝑟𝑎𝑡𝑜𝑟 𝐷𝑢𝑡𝑦
𝐶𝑜𝑚𝑝𝑟𝑒𝑠𝑠𝑜𝑟 𝐷𝑢𝑡𝑦
𝐶𝑂𝑃 =
𝑇𝑒
𝑇𝑐 − 𝑇𝑒
Refrigerant
Temperature
Variables
Upper bound
(C)
Lower bound (C)
Optimized value
(C)
Carnot COP Correction factor Actual COP
i-butane
Evaporator
temperature
5 -5 -5
8.579 0.706 6.053
Condenser
temperature
39.89 26.24 26.24
NH3
Evaporator
temperature
5 -5 5
12.64 0.434 5.492
Condenser
temperature
39.67 26.81 26.81
R1234yf
Evaporator
temperature
5 -7 -7
8.313 0.576 4.785
Condenser
temperature
48.23 28.01 28.01
CO2
Evaporator
temperature
6 -1 6
13.24 0.331 4.38
Condenser
temperature
32 27.08 27.08
• Natural refrigerants are an environmentally friendly alternative to synthetic refrigerants
owing to their low ODP and GWP.
• A comparison among the four natural refrigerants shows that ammonia has the highest COP
followed by the two hydrocarbons (iso-butane and R1234yf), and CO2 has the least COP.
• The sensitivity analysis shows that the condenser temperature has a greater influence on the
COP than the evaporator temperature
• In the optimization studies, COP was maximized by adjusting the condenser and evaporator
temperatures.
CONCLUSIONS
THANK YOU

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Modelling and Simulation systems PRESENTATION.pptx

  • 1. MODELLING AND SIMULATION OF NATURAL REFRIGERATION SYSTEMS EXTERNAL GUIDE: Dr.SUNIL SHAH (CEO Modelicon InfoTech LLP) EVAN AALEX 1MS20CH016 NEHA S PATWARDHAN 1MS20CH024 SARAH FATIMA 1MS20CH030 VISHWANATH SABARAD 1MS20CH043 DEPARTMENT OF CHEMICAL ENGINEERING PROJECT GUIDE: Dr.BRIJESH
  • 2. TABLE OF CONTENTS 1. Scope 2. Objectives 3. Introduction 4. Vapour Compression Refrigeration Cycle 5. Modelling and Simulation 6. Results and Discussions • COP and Flow rate trends • Comparison based on COP • Sensitivity analysis • Optimization 7. Conclusion
  • 3. Comparison of refrigerants based on factors such as environmental impact, safety considerations, application specificity, cost and energy consumption helps in selection of the best suited model for the respective application. SIMULATION • To optimize the design and maximize the system efficiency by minimizing energy consumption and operating cost. • To scale up the process. The global green refrigerants market was valued at US$ 18.8 billion in 2022 and is expected to reach US$ 32.1 billion by 2030. FUTURE OF REFRIGERANTS • Predict refrigeration system performance with respect to parameters such as cooling capacity, COP, temperature etc. • Process optimization by adjusting parameters such as flow rate, pressure ratio, temperature etc. MODELLING COMPARISON SCOPE
  • 4. OBJECTIVES  Model and simulate a simple refrigeration loop for each of the four fluids – carbon dioxide, ammonia, isobutane, and 2,3,3,3-tetrafluoropropene (R1234yf) using Aspen HYSYS.  Analyse the refrigeration loops over a range of operating conditions and conduct sensitivity analysis.  Compare these models on the basis of their performance.  Optimize each refrigeration loop to maximize COP
  • 5. INTRODUCTION • Refrigeration technology plays an important role in various industries • 15–20% of the world’s electricity is used by refrigeration (Yatangababa et al., 2015) • Most synthetic refrigerants, released into the atmosphere cause depletion of ozone layer and global warming. • Natural refrigerants have low or no GWP and ODP. (Cavallini 2020; Abas et al.,2018)
  • 6. REFIGERANTS AND THEIR PROPERTIES Refrigerant R717 R744 R600a R1234yf Chemical Formula NH3 CO2 CH(CH3)2CH3 CF3CF=CH2 GWP <1 1 4 <1 ODP 0 0 0 0 Critical Pressure (MPa) 11.33 7.38 3.64 3.4 Critical Temperature (oC) 132.2 31.1 134.7 94.7 Normal Boiling Point (oC) -33 -78.4 -11.7 -29.54 Specific Heat capacity (kJ/kg-K) 4.7 0.63 2.4 1.39 Latent Heat (kJ/kg) 1370 571.0 345.83 180.25 ASHRAE safety group A1 A1 A3 A2L ASHRAE flammability No No Yes (high) Yes (mild) ASHRAE toxicity Yes No No No • Ammonia – R717 • Carbon Dioxide – R744 • Isobutane – R600a • 2,3,3,3-Tetrafluoropropene – R1234yf (Kyriakides et al.,2020)
  • 7. VAPOUR COMPRESSION REFRIGERATION SYSTEMS (VCRS) VCRS mainly consists of – Chilled fluid Fluid EVAPORATOR CONDENSER COMPRESSOR VALVE Cooling fluid Evaporator: Heat is absorbed from the medium to be cooled. Refrigerant evaporates. Compressor: Refrigerant is compressed to high temperature and pressure. Compressor circulates the refrigerant. Condenser: Refrigerant gives up heat and is condensed to a liquid. Expansion valve: High-pressure refrigerant expands to low temperature and pressure.
  • 8. Specifications Value Unit Chiller Capacity 200 kW Chiller water inlet Temperature 12 ℃ Chiller water outlet Temperature 7 ℃ Evaporator Superheat 0, 1, 2 ℃ Cooling water inlet Temperature (Condenser) 24 ℃ Cooling water outlet Temperature (Condenser) 28 ℃ Table 1: Process conditions of the simulation Process flow sheet
  • 9. STEADY STATE MODELLING Equipment Parameter Equation Evaporator Heat Balance (kW) Q=m Cp ∆T Compressor Work done (kW) Volumetric Capacity (m3/hr) 𝑊 = 𝑧𝑅𝑇 𝛾 𝛾 − 1 [( 𝑃𝑑 𝑃𝑠 ) 𝛾−1 𝛾 − 1] × 𝑚 𝑉 = 𝑚 𝜌 Condenser Heat Balance (kW) Q=m Cp ∆T Expansion Valve Pressure Drop (kPa) Δ𝑃 = Δ𝐻 𝜌. 𝑔. 𝜂 Overall System Coefficient of Performance (COP) Carnot COP 𝐶𝑂𝑃 = 𝐸𝑣𝑎𝑝𝑜𝑟𝑎𝑡𝑜𝑟 𝐷𝑢𝑡𝑦 𝐶𝑜𝑚𝑝𝑟𝑒𝑠𝑠𝑜𝑟 𝐷𝑢𝑡𝑦 𝐶𝑂𝑃 = 𝑇𝑒 𝑇𝑐 − 𝑇𝑒 Q – heat rate (kW) m – mass flowrate (kg/h) Cp – Constant pressure specific heat capacity T – absolute temperature (K) z – compressibility factor R – universal gas constant (J/mol-K) Pd – Discharge pressure Ps – suction pressure 𝜌 – density of fluid (kg/m3) 𝛾 – adiabatic index 𝜂 – adiabatic efficiency Te − Evaporator temperature (K) Tc – condenser temperature (K)
  • 10. SIMULATION 1. SETTING THE PROPERTIES 2. SIMULATION ENVIRONMENT • Four components • Peng-Robinson fluid package Heat exchangers • Tube side – water, Shell side – refrigerant • Pressure drop • Chilling water flow rate = 33350 kg/hr • Inlet and outlet temperatures Compressor • Efficiency = 75% • Pressure ratio = 3
  • 12. 0 2 4 6 8 10 -15 -10 -5 0 5 10 COP Evaporation Temperature (°C) Carbon dioxide Tc = 30 ℃ Tc = 25 ℃ Tc = 20 ℃ 0 1 2 3 4 5 6 7 8 -40 -30 -20 -10 0 10 COP Evaporation temperature (℃) Ammonia Tc = 30℃ Tc = 35℃ Tc = 40℃ Tc = 45℃ 0 1 2 3 4 5 6 -7.5 -5 -2.5 0 2.5 5 7.5 COP Evaporation Temperature (℃) R1234yf Tc = 40 ℃ Tc = 45 ℃ Tc = 50 ℃ Tc = 55 ℃ 0 1 2 3 4 5 6 7 8 -40 -30 -20 -10 0 10 COP Evaporation temperature (C) Iso-butane Tc = 30 ℃ Tc = 35 ℃ Tc = 40 ℃ Tc = 45 ℃ COP vs Evaporator Temperature
  • 13. Mass flow rate vs Evaporator Temperature 0.00 5000.00 10000.00 15000.00 20000.00 25000.00 -40 -30 -20 -10 0 10 Mass Flowrate (kg/hr) Evaporator Temperature (⁰C) R-1234yf Tc = 30 ⁰C Tc = 35 ⁰C Tc = 40 ⁰C Tc = 45 ⁰C
  • 14. 0 2000 4000 6000 8000 10000 12000 14000 16000 0 10 20 30 40 Flow rate (kg/hr) Evaporator duty (kJ/hr) x 100000 Isobutane 0 20000 40000 60000 80000 100000 0 300 600 900 1200 Flowrate (kg/hr) Evaporator Duty (kJ/hr) x 100000 Ammonia R1234yf Carbon Dioxide Mass flowrate vs Evaporator Duty
  • 15. COMPARISON Ammonia – Better thermodynamic properties Iso-butane – hydrocarbon R1234yf – hydrocarbon Carbon dioxide – subcritical state
  • 17. OPTIMIZATION 𝐶𝑂𝑃 = 𝐸𝑣𝑎𝑝𝑜𝑟𝑎𝑡𝑜𝑟 𝐷𝑢𝑡𝑦 𝐶𝑜𝑚𝑝𝑟𝑒𝑠𝑠𝑜𝑟 𝐷𝑢𝑡𝑦 𝐶𝑂𝑃 = 𝑇𝑒 𝑇𝑐 − 𝑇𝑒 Refrigerant Temperature Variables Upper bound (C) Lower bound (C) Optimized value (C) Carnot COP Correction factor Actual COP i-butane Evaporator temperature 5 -5 -5 8.579 0.706 6.053 Condenser temperature 39.89 26.24 26.24 NH3 Evaporator temperature 5 -5 5 12.64 0.434 5.492 Condenser temperature 39.67 26.81 26.81 R1234yf Evaporator temperature 5 -7 -7 8.313 0.576 4.785 Condenser temperature 48.23 28.01 28.01 CO2 Evaporator temperature 6 -1 6 13.24 0.331 4.38 Condenser temperature 32 27.08 27.08
  • 18. • Natural refrigerants are an environmentally friendly alternative to synthetic refrigerants owing to their low ODP and GWP. • A comparison among the four natural refrigerants shows that ammonia has the highest COP followed by the two hydrocarbons (iso-butane and R1234yf), and CO2 has the least COP. • The sensitivity analysis shows that the condenser temperature has a greater influence on the COP than the evaporator temperature • In the optimization studies, COP was maximized by adjusting the condenser and evaporator temperatures. CONCLUSIONS