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Cheatsheet: Refrigeration Cycles

1. Vapor-Compression Refrigeration Cycle

1.1 Ideal Cycle Components and Processes

Process Description
1-2: Isentropic Compression Compressor increases pressure and temperature of refrigerant vapor; s₁ = s₂
2-3: Constant Pressure Condensation Refrigerant rejects heat to surroundings in condenser; exits as saturated liquid
3-4: Throttling (Isenthalpic) Expansion valve reduces pressure; h₃ = h₄; quality increases
4-1: Constant Pressure Evaporation Refrigerant absorbs heat from cold space in evaporator; exits as saturated vapor

1.2 Performance Parameters

Parameter Formula
Coefficient of Performance (COP) COP = QL/Wnet = (h₁ - h₄)/(h₂ - h₁)
Refrigeration Effect QL = ṁ(h₁ - h₄)
Compressor Work Wcomp = ṁ(h₂ - h₁)
Heat Rejected QH = ṁ(h₂ - h₃)
Refrigeration Capacity Expressed in tons (1 ton = 12,000 Btu/hr = 3.517 kW)

1.3 Actual Cycle Deviations

  • Compression: Non-isentropic due to irreversibilities; isentropic efficiency ηc = (h₂s - h₁)/(h₂a - h₁)
  • Pressure drops in evaporator and condenser due to friction
  • Heat transfer to/from surroundings in connecting pipes
  • Subcooling of liquid leaving condenser increases COP
  • Superheating of vapor entering compressor protects compressor from liquid droplets

2. Refrigerant Properties and Selection

2.1 Common Refrigerants

Refrigerant Key Characteristics
R-134a Automotive and residential AC; replaced R-12; GWP = 1430; non-toxic, non-flammable
R-410A Residential/commercial AC; replaced R-22; zeotropic blend; higher pressure than R-22
R-22 Being phased out (HCFC); ODP = 0.055; formerly common in AC
R-717 (Ammonia) Industrial refrigeration; excellent thermodynamic properties; toxic but natural refrigerant
R-744 (CO₂) Natural refrigerant; low GWP; requires high operating pressures; transcritical cycles

2.2 Selection Criteria

  • Thermodynamic performance: high latent heat, suitable pressure range
  • Environmental impact: Ozone Depletion Potential (ODP), Global Warming Potential (GWP)
  • Safety: toxicity, flammability classification (ASHRAE 34)
  • Chemical stability and compatibility with materials
  • Cost and availability

3. Absorption Refrigeration Systems

3.1 Basic Absorption Cycle

Component Function
Absorber Refrigerant vapor absorbed by solution; heat rejected QA
Pump Pumps rich solution to high pressure; work input minimal (Wpump ≪ Wcomp)
Generator Heat input QG drives refrigerant from solution; produces weak solution
Condenser Refrigerant vapor condenses; heat rejected QC
Expansion Valve Throttles liquid refrigerant to low pressure
Evaporator Refrigerant evaporates; absorbs heat QE from cold space

3.2 Performance and Working Pairs

Parameter Definition/Value
COPabsorption COP = QE/QG (heat-driven; range 0.6-0.8)
H₂O-LiBr System Water is refrigerant, lithium bromide is absorbent; used for AC; limited to T > 0°C
NH₃-H₂O System Ammonia is refrigerant, water is absorbent; industrial refrigeration; rectifier needed

3.3 Advantages and Applications

  • Heat source can be waste heat, solar, or natural gas
  • Fewer moving parts than vapor-compression systems
  • Quiet operation
  • Used in applications where electricity is expensive or heat is available

4. Multistage and Cascade Refrigeration

4.1 Multistage Compression

Feature Description
Purpose Reduces compressor work and discharge temperature for large pressure ratios
Optimal Interstage Pressure Pint = √(Plow × Phigh) for two-stage
Flash Chamber Separates liquid and vapor between stages; improves efficiency
Intercooling Cools refrigerant between compression stages; approaches isothermal compression

4.2 Cascade Refrigeration

  • Two or more separate refrigeration cycles in series
  • Evaporator of higher-temperature cycle cools condenser of lower-temperature cycle
  • Different refrigerants in each cycle optimized for temperature range
  • Used for very low temperatures (T <>
  • COPcascade = COP₁ × COP₂/(COP₁ + COP₂ + 1)

5. Modified Vapor-Compression Cycles

5.1 Cycle Enhancements

Modification Benefit
Liquid Subcooling Increases refrigeration effect; reduces quality entering evaporator
Vapor Superheating Prevents liquid carryover to compressor; may decrease COP if excessive
Suction Line Heat Exchanger Subcools liquid with cold suction vapor; increases h₁, decreases h₄

5.2 Heat Pump Operation

Parameter Formula/Description
COPHP COPHP = QH/Wnet = (h₂ - h₃)/(h₂ - h₁)
Relationship COPHP = COPR + 1
Application Space heating; reversible operation for heating/cooling

6. Air-Conditioning Systems

6.1 Psychrometric Properties

Property Definition
Dry Bulb Temperature (DBT) Temperature measured by standard thermometer
Wet Bulb Temperature (WBT) Temperature with evaporative cooling; constant enthalpy lines on chart
Dew Point Temperature Temperature at which condensation begins at constant humidity ratio
Relative Humidity (φ) φ = Pv/Pg where Pv is vapor pressure, Pg is saturation pressure
Humidity Ratio (ω) ω = 0.622 × Pv/(P - Pv) in lbv/lbda or kgv/kgda
Specific Enthalpy h = cpT + ωhfg where cp ≈ 1.005 kJ/kg·K for dry air

6.2 Air-Conditioning Processes

Process Characteristics
Sensible Heating/Cooling Constant humidity ratio (horizontal line on chart); changes temperature only
Humidification Increases moisture content; steam injection (constant DBT) or evaporative (constant WBT)
Dehumidification Cooling below dew point; condensate removed; decreases both T and ω
Adiabatic Mixing h₃ = (ṁ₁h₁ + ṁ₂h₂)/(ṁ₁ + ṁ₂); ω₃ = (ṁ₁ω₁ + ṁ₂ω₂)/(ṁ₁ + ṁ₂)

6.3 Load Calculations

  • Sensible Heat Ratio (SHR) = Qsensible/Qtotal
  • Cooling load: Qsensible = ṁacp(T₁ - T₂); Qlatent = ṁahfg(ω₁ - ω₂)
  • Bypass Factor (BF) = (T₂ - Tcoil)/(T₁ - Tcoil); indicates coil effectiveness
  • Apparatus Dew Point (ADP): effective surface temperature of cooling coil

7. Gas Refrigeration Cycles

7.1 Reversed Brayton Cycle

Process Description
1-2: Isentropic Compression Compressor increases gas pressure and temperature
2-3: Constant Pressure Cooling Heat exchanger rejects heat to surroundings
3-4: Isentropic Expansion Expander (turbine) reduces temperature below T₁
4-1: Constant Pressure Heating Refrigerated space adds heat to gas

7.2 Performance

  • COP = 1/(rp(γ-1)/γ - 1) where rp = P₂/P₁ is pressure ratio
  • Uses air or helium as working fluid
  • Lower COP than vapor-compression but operates at very low temperatures
  • No phase change; continuous gas operation
  • Applications: aircraft AC, cryogenic systems, liquefaction processes

8. Thermodynamic Analysis

8.1 First Law Analysis

Component Energy Balance
Compressor Wcomp = ṁ(h₂ - h₁); for isentropic: ηc = (h₂s - h₁)/(h₂a - h₁)
Condenser Qout = ṁ(h₂ - h₃)
Expansion Valve h₃ = h₄ (isenthalpic throttling)
Evaporator Qin = ṁ(h₁ - h₄)

8.2 Second Law Analysis

  • Carnot COPR = TL/(TH - TL); maximum theoretical efficiency
  • Carnot COPHP = TH/(TH - TL)
  • Exergy destruction identifies irreversibilities in each component
  • Throttling valve: major source of irreversibility (Δs > 0, Δh = 0)
  • Second law efficiency: ηII = COPactual/COPCarnot

8.3 Key Performance Metrics

Metric Expression
Energy Efficiency Ratio (EER) EER = Qcooling (Btu/hr) / Winput (W)
Seasonal EER (SEER) Cooling output over season / Total electrical input; accounts for part-load
Heating Seasonal Performance Factor HSPF = Total heating output (Btu) / Total electrical input (W·hr)

9. Refrigeration System Components

9.1 Compressor Types

Type Characteristics
Reciprocating Positive displacement; piston-cylinder; 1-1500 tons; capacity control via cylinder unloading
Rotary (Scroll) Positive displacement; two spiral scrolls; 2-20 tons; smooth operation, high efficiency
Screw Positive displacement; helical rotors; 20-750 tons; continuous compression, oil-cooled
Centrifugal Dynamic; impeller accelerates refrigerant; >100 tons; high flow, low pressure ratio per stage

9.2 Heat Exchangers

  • Evaporator types: direct expansion (DX), flooded, shell-and-tube
  • Condenser types: air-cooled (finned tube), water-cooled (shell-and-tube), evaporative
  • Effectiveness-NTU method: ε = (actual heat transfer)/(maximum possible heat transfer)
  • Log Mean Temperature Difference: LMTD = (ΔT₁ - ΔT₂)/ln(ΔT₁/ΔT₂)
  • Heat transfer: Q = UA × LMTD where U is overall heat transfer coefficient

9.3 Expansion Devices

Device Application
Thermostatic Expansion Valve Modulates flow based on superheat at evaporator exit; maintains constant superheat
Capillary Tube Fixed restriction; simple, no moving parts; limited to small systems with constant load
Electronic Expansion Valve Precise control via sensors and controller; optimal for variable load applications
Float Valve Maintains liquid level in evaporator; used in flooded evaporators

10. Special Applications and Considerations

10.1 Low-Temperature Refrigeration

  • Cascade systems required for T <>
  • Auto-refrigerating cascade uses mixed refrigerants
  • Cryogenic systems: T < -150°c;="" use="" gas="" cycles="" or="" joule-thomson="">
  • Liquefaction: Linde cycle (simple throttling), Claude cycle (expander)

10.2 Capacity Control Methods

Method Description
On-Off Control Simple cycling; large temperature swings; low cost
Hot Gas Bypass Redirects discharge gas to evaporator inlet; reduces capacity without cycling
Variable Speed Drive Varies compressor speed; excellent efficiency at part-load; higher cost
Cylinder Unloading Deactivates cylinders in reciprocating compressors; stepped capacity reduction

10.3 Refrigeration Safety

  • ASHRAE 34: refrigerant safety classification (toxicity: A/B; flammability: 1/2L/2/3)
  • Pressure relief devices required on all pressure vessels
  • Refrigerant leak detection and monitoring systems
  • Maximum discharge temperature limits to prevent oil breakdown (~150°C for mineral oil)
  • Evacuation and charging procedures per EPA regulations
The document Cheatsheet: Refrigeration Cycles is a part of the PE Exam Course Mechanical Engineering for PE.
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