UNIT 5: REFRIGERATION & AIR CONDITIONING - SHORT NOTES
Based on analysis of past examination papers (Jun 2025, May 2024, May 2023, May 2022).
1.0 FUNDAMENTAL CONCEPTS & PERFORMANCE METRICS
1.1 Tonne of Refrigeration (TR)
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Definition: The amount of refrigeration effect required to produce 1 tonne (1000 kg) of ice at 0°C from liquid water at 0°C in 24 hours.
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Numerical Value:
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$$\displaystyle 1 \text{ TR} = 3.517 \text{ kW} $$
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$$\displaystyle 1 \text{ TR} = 12000 \text{ Btu/h} $$
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Calculation Basis: Latent heat of ice = 335 kJ/kg.
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Refrigeration required per day = $$\displaystyle 1000 \text{ kg} \times 335 \text{ kJ/kg} = 335,000 \text{ kJ} $$
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Refrigeration per hour = $$\displaystyle \frac{335,000}{24} \approx 13,958 \text{ kJ/h} \approx 3.877 \text{ kW} $$.
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Standard value adopted: 3.517 kW (based on older imperial definition).
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Exam Problems: Used to find mass of ice produced, power input, or COP when capacity in TR is given.
1.2 Coefficient of Performance (COP)
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Definition: Ratio of desired effect (refrigeration or heating) to the work input required.
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Refrigerator/Heat Pump: $$\displaystyle \text{COP} = \frac{\text{Refrigeration Effect (} Q_L \text{)}}{\text{Net Work Input (} W_{net} \text{)}} $$
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Heat Engine: $$\displaystyle \text{COP (or Efficiency)} = \frac{\text{Net Work Output}}{\text{Heat Input}} = \frac{W_{net}}{Q_H} $$
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Carnot COP (Reversible Cycle):
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Refrigerator/Heat Pump: $$\displaystyle \text{COP}_{\text{Carnot}} = \frac{T_L}{T_H - T_L} $$
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Heat Engine: $$\displaystyle \eta_{\text{Carnot}} = 1 - \frac{T_L}{T_H} $$
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Where $$\displaystyle T_L $$ = Lowest absolute temperature (evaporator), $$\displaystyle T_H $$ = Highest absolute temperature (condenser).
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Relationship: For same $$\displaystyle T_L $$ and $$\displaystyle T_H $$, $$\displaystyle \text{COP}_{\text{HP}} = \text{COP}_{\text{Ref}} + 1 $$.
1.3 Refrigeration Effect & Capacity
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Refrigeration Effect ($$\displaystyle q_L $$): Amount of heat absorbed in the evaporator per kg of refrigerant. (kJ/kg)
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Capacity: Rate of refrigeration.
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$$\displaystyle \text{Capacity (kW)} = \dot{m}_r \times q_L $$
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$$\displaystyle \text{Capacity (TR)} = \frac{\dot{m}_r \times q_L}{3.517} $$
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Where $$\displaystyle \dot{m}_r $$ = mass flow rate of refrigerant (kg/s).
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[!TIP]
Common Pitfall: Confusing COP with Efficiency. COP can be >1 for refrigeration/heat pumps; efficiency for heat engines is always <1. Always use absolute temperatures (K) for Carnot COP.
2.0 VAPOUR COMPRESSION REFRIGERATION SYSTEMS (VCRS)
2.1 Theoretical (Ideal) Cycle
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Processes (on P-h, T-S diagrams):
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1-2: Isentropic compression (s1 = s2).
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2-3: Constant pressure condensation (heat rejection $$\displaystyle Q_H $$).
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3-4: Throttling (isenthalpic, h3 = h4).
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4-1: Constant pressure evaporation (heat absorption $$\displaystyle Q_L $$).
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COP Expression: $$\displaystyle \text{COP} = \frac{h_1 - h_4}{h_2 - h_1} $$
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$$\displaystyle h_1 $$ = enthalpy at evaporator exit (compressor inlet).
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$$\displaystyle h_2 $$ = enthalpy at compressor exit.
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$$\displaystyle h_3 $$ = enthalpy at condenser exit.
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$$\displaystyle h_4 = h_3 $$ (throttling).
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2.2 Practical (Actual) Cycle
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Superheating (1-1'): Vapour at compressor inlet is superheated.
- Effect: Increases refrigeration effect ($$\displaystyle h_1' - h_4 $$) and compressor work ($$\displaystyle h_2' - h_1' $$). Net effect on COP depends on degree of superheat.
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Sub-cooling (Undercooling) (3-3'): Liquid at condenser exit is cooled below saturation temperature.
- Effect: Increases refrigeration effect ($$\displaystyle h_1 - h_4' $$) without increasing compressor work. Improves COP.
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Effect of Pressures:
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Lower Suction Pressure (Lower $$\displaystyle T_{evap} $$): Decreases refrigeration effect per kg, increases compressor work ratio → COP decreases, capacity decreases.
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Higher Discharge Pressure (Higher $$\displaystyle T_{cond} $$): Increases compressor work, decreases refrigeration effect → COP decreases.
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Volumetric Efficiency ($$\displaystyle \eta_v $$): $$\displaystyle \eta_v = \frac{\text{Actual volume sucked}}{\text{Piston displacement volume}} $$. Affects effective capacity.
2.3 P-H (Pressure-Enthalpy) Chart
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Construction: Pressure (log scale) vs. Enthalpy. Shows saturation dome (liquid-vapour region).
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Interpretation:
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Left of dome: compressed liquid.
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Right of dome: superheated vapour.
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Inside dome: wet vapour (quality $x$).
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Constant temperature lines (isotherms) are horizontal in wet region.
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Constant entropy lines (isentropes) are vertical in wet region.
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Plotting Cycle: Locate points 1 (evap exit), 2 (comp exit, isentropic from 1), 3 (cond exit), 4 (throttle from 3, h4=h3).
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Determining Properties: Read $h$, $P$, $T$, quality from chart.
2.4 Multistage Compression
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Need: High pressure ratios cause high discharge temperature, low volumetric efficiency, high work input.
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Liquid Intercooler:
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Function: Cool the refrigerant liquid between stages (after condenser of high stage, before entering low-stage evaporator or as separate exchanger).
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Advantages:
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Reduces compressor work (lower $T$ at inlet to second stage).
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Improves lubrication (lower discharge temp).
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Reduces discharge temperature.
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Increases refrigeration effect (sub-cooling effect).
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Boot-strap Cycle (Flash Intercooling):
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Principle: Use a flash chamber after high-stage compression. Part of high-pressure liquid flashes to vapour, cooling the remaining liquid. The vapour is routed to the low-stage compressor inlet.
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Working: High-stage discharge → Flash chamber → Liquid (to expansion valve) + Vapour (to low-stage suction).
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COP Expression: $$\displaystyle \text{COP} = \frac{h_1 - h_4}{(h_2 - h_1) + (h_5 - h_4)} $$ (for two-stage with flash intercooling, where 5 is low-stage inlet from flash chamber).
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2.5 Cascade Refrigeration Systems
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Definition: Two or more independent vapour compression cycles operating at different pressure levels, coupled via a cascade heat exchanger.
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Necessity: To achieve very low temperatures (below -80°C) where single-stage compression is inefficient or impractical.
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Comparison with Multistage:
| Feature | Multistage Compression | Cascade System | | :--- | :--- | :--- | | Compressors | Multiple stages in series, often same refrigerant | Separate compressors, different refrigerants common | | Circuit | Single continuous refrigerant circuit | Multiple independent circuits | | Inter-stage Cooling | Intercooler (liquid or flash) | Cascade heat exchanger (condenser of low cycle = evaporator of high cycle) | | Flexibility | Less flexible | More flexible (can optimize each stage) | | Complexity | Lower | Higher (more components, controls) |
[!TIP]
Key Difference: In multistage, refrigerant is same throughout; in cascade, different refrigerants can be used for low/high stages (e.g., R-23 for low, R-404A for high).
3.0 VAPOUR ABSORPTION REFRIGERATION SYSTEMS (VARS)
3.1 Basic Principle & Comparison with VCRS
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VCRS: Uses a compressor to increase pressure and temperature of refrigerant vapour. Requires significant mechanical work.
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VARS: Replaces compressor with absorber and generator.
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Absorber: Low-pressure refrigerant vapour is absorbed by a liquid absorbent (e.g., NH₃ into H₂O). This creates a low-pressure solution.
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Generator: The strong solution is pumped to a high-pressure generator and heated (by waste heat, steam, etc.). Refrigerant vapour is driven off at high pressure.
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Pump: Requires little work to circulate the liquid solution (vs. compressing vapour).
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Advantages of VARS:
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Utilizes low-grade thermal energy (waste heat, solar).
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Quiet operation (no moving parts in vapour circuit).
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Can be used where electricity is scarce/expensive.
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3.2 Practical Vapour Absorption Cycle (Aqua-Ammonia)
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Components:
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Generator: Heat input → strong NH₃-H₂O solution → high-pressure NH₃ vapour + weak solution.
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Condenser: NH₃ vapour condenses to liquid.
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Evaporator: Liquid NH₃ evaporates at low pressure → refrigeration effect.
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Absorber: Evaporated NH₃ vapour absorbed by cool water → strong solution.
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Solution Pump: Pressurizes strong solution to generator pressure.
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Throttle Valve: Weak solution from generator to absorber.
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Heat Exchanger (optional): Economizer to pre-heat strong solution / cool weak solution.
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Working: Follows the path on T-s or P-h diagram: 1 (weak sol) → 2 (strong sol, pump) → 3 (vapour + weak sol, generator) → 4 (liquid, condenser) → 5 (vapour, evaporator) → 6 (strong sol, absorber).
3.3 Refrigerant-Absorbent Combination
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Desirable Properties:
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High affinity (refrigerant readily absorbed).
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Large difference in boiling points (refrigerant boils off easily in generator).
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Low viscosity, high thermal conductivity.
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Chemical stability (no decomposition).
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Non-corrosive.
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Low freezing point (for absorbent).
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Low vapour pressure at operating temperatures (for absorbent).
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Common Pairs:
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Ammonia (Refrigerant) - Water (Absorbent): Most common for industrial/commercial. High COP.
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Lithium Bromide (Absorbent) - Water (Refrigerant): Used for large building AC. Requires vacuum operation, risk of crystallization.
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4.0 AIR REFRIGERATION SYSTEMS (Dense Air Cycle)
4.1 Dense Air vs. Open Air System
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Dense Air (Closed) Cycle: Air is compressed, cooled, expanded in a turbine (or throttled), then cooled in the evaporator. Air is re-circulated in a closed loop. Used in aircraft.
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Open Air Cycle: Ambient air is compressed, cooled, expanded, and ejected overboard. Simple but inefficient.
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Advantages of Dense Air System:
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No loss of refrigerant (air).
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Can maintain cabin pressure independently.
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More efficient than open cycle (uses expansion work).
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4.2 Aircraft Refrigeration Systems
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Need: At high altitude, ambient air is very cold but at low pressure. Cabin must be pressurized and cooled.
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Process: Ambient air → Ram effect (compression due to aircraft speed) → Main compressor → Heat exchanger (cooling with ambient air) → Turbine (expansion to cabin pressure, produces cooling) → Cabin.
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Calculations (per kg/s of air flow):
- Power for Pressurization ($$\displaystyle W_p $$): Work to compress air from ambient pressure $$\displaystyle P_a $$ to cabin pressure $$\displaystyle P_c $$.
$$W_p = C_p (T_2 - T_1)$$
(Isentropic compression from state 1 to $$\displaystyle P_c $$, then cooling to $$\displaystyle T_2 $$).
2. **Additional Power for Refrigeration ($$\displaystyle W_t $$):** Work extracted in turbine to expand from $$\displaystyle P_c $$ to $$\displaystyle P_a $$.
$$W_t = C_p (T_3 - T_4)$$
(Isentropic expansion from state 3 to $$\displaystyle P_a $$).
3. **Net Power Input:** $$\displaystyle W_{net} = W_p - W_t $$ (if turbine drives compressor) or total if separate.
4. **Refrigerating Effect ($$\displaystyle q_L $$):** $$\displaystyle q_L = C_p (T_4 - T_{ambient}) $$ or $$\displaystyle C_p (T_4 - T_5) $$ where $$\displaystyle T_5 $$ is supply air temp.
- Key Point: Air acts as the refrigerant in a reversed Brayton (Bell Coleman) cycle.
5.0 REFRIGERANTS
5.1 Classification
| Category | Description | Examples |
|---|---|---|
| Primary | Used in vapour compression/absorption cycles. Undergo phase change. | R-12, R-22, NH₃, CO₂, R-134a |
| Secondary | Used in single-phase circulation (brines, glycols). | Water, Ethylene Glycol, Calcium Chloride brine |
| CFCs | Chlorofluorocarbons (Ozone Depleting). | R-11, R-12, R-113 |
| HCFCs | Hydrochlorofluorocarbons (Partial ODP). | R-22, R-123 |
| HFCs | Hydrofluorocarbons (Zero ODP, high GWP). | R-134a, R-404A, R-410A |
| HFOs | Hydrofluoroolefins (Zero ODP, low GWP). | R-1234yf, R-1234ze |
| Natural | Occur in nature, environmentally benign. | NH₃ (R-717), CO₂ (R-744), Propane (R-290), Isobutane (R-600a) |
5.2 Desirable Properties of an Ideal Refrigerant
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Low boiling point (at atmospheric pressure).
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High latent heat of vaporization (large refrigeration effect per kg).
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Low specific volume (reduces compressor size).
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Non-toxic, non-flammable, non-explosive.
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Chemically stable (no decomposition under operating conditions).
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Good thermal conductivity (improves heat exchanger performance).
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Miscible with lubricating oil (ensures proper lubrication).
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Low cost and easily available.
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Zero ODP and low GWP (modern requirement).
5.3 Selection Factors
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Safety: Toxicity, flammability, explosiveness.
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Environmental Impact: ODP (Ozone Depletion Potential), GWP (Global Warming Potential).
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Thermodynamic Properties: Critical temperature, pressure, latent heat, specific heat.
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Compatibility: With materials (metals, elastomers), lubricating oil.
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Cost & Availability.
5.4 Specific Refrigerants
| Refrigerant | Chemical Formula | ASHRAE No. | Properties & Applications |
|---|---|---|---|
| Ammonia | NH₃ | R-717 | Properties: High latent heat, good thermodynamic properties, toxic, flammable, strong odor. Applications: Industrial refrigeration, cold storages. |
| R-12 | CCl₂F₂ | R-12 | Properties: Non-toxic, non-flammable, stable. High ODP (1.0), high GWP. Applications: Historically domestic/commercial refrigeration, AC. Phased out globally. |
| R-22 | CHClF₂ | R-22 | Properties: Non-toxic, non-flammable. ODP ~0.05, moderate GWP. Applications: Air conditioning (residential, commercial). Being phased out (Montreal Protocol). |
- ASHRAE Numbering: e.g., CHClF₂ → R-22 (add 90 to number of H atoms: 1+90=91, subtract Cl atoms: 91-2=89? Actually standard: CHClF₂ has 1 C, 1 H, 1 Cl, 2 F → R-22. Rule: For methane-based, R(Number of H atoms + 90) - (Number of Cl atoms) - (Number of Br atoms) etc. Simplified: CHClF₂ → 1 H → 91, minus 1 Cl → 90? Wait, standard is R-22. Better to memorize common ones: R-12=CCl2F2, R-22=CHClF2, R-134a=CH2FCF3.*
5.5 Environment-Friendly Refrigerants
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Alternatives to CFCs/HCFCs:
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HFCs: Zero ODP, but high GWP (e.g., R-134a, R-410A).
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HFOs: Zero ODP, very low GWP (e.g., R-1234yf for car AC).
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Natural Refrigerants: NH₃ (R-717), CO₂ (R-744), Hydrocarbons (R-290, R-600a). Very low GWP, but may have toxicity/flammability.
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Concepts:
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ODP (Ozone Depletion Potential): Relative to R-11 (ODP=1). Measures potential to destroy stratospheric ozone.
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GWP (Global Warming Potential): Relative to CO₂ (GWP=1) over 100 years. Measures contribution to climate change.
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6.0 PSYCHROMETRY & AIR CONDITIONING PROCESSES
6.1 Psychrometric Terms & Chart
| Term | Symbol | Definition |
|---|---|---|
| Dry Bulb Temperature (DBT) | $t$ or $$\displaystyle T_{db} $$ | Measured by ordinary thermometer. |
| Wet Bulb Temperature (WBT) | $$\displaystyle t_{wb} $$ | Temperature read by thermometer with wet wick. Indicates moisture content. |
| Dew Point Temperature | $$\displaystyle t_{dp} $$ | Temperature at which air becomes saturated (RH=100%) when cooled at constant pressure. |
| Relative Humidity (RH) | $\phi$ | $$\displaystyle \phi = \frac{\text{Partial pressure of vapour}}{\text{Saturation vapour pressure at DBT}} \times 100\% $$ |
| Specific Humidity (Humidity Ratio) | $\omega$ | $$\displaystyle \omega = 0.622 \frac{p_v}{p - p_v} $$ (kg water/kg dry air). |
| Saturated Air | - | Air containing maximum water vapour possible at given DBT (RH=100%). |
| Enthalpy of moist air | $h$ | $$\displaystyle h = 1.005 t + \omega (2501 + 1.88 t) $$ kJ/kg dry air. |
- Psychrometric Chart: Plot of $\omega$ vs. $t$. Lines: constant RH (curved), constant $h$ (straight, sloped), constant WBT (approx. straight), constant volume (approx. straight).
6.2 Psychrometric Processes on Chart
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Sensible Heating/Cooling: Constant $\omega$ (horizontal line). Heat added/removed: $$\displaystyle Q_s = m_a C_{pa} \Delta t $$.
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Humidification (Adding Moisture): $\omega$ increases. Usually constant $t$ (vertical up) or constant WBT.
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Dehumidification (Removing Moisture): $\omega$ decreases. Usually constant $t$ (vertical down) or constant WBT.
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Heating & Humidification: Combination (right/up).
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Cooling & Dehumidification: Most common in AC. Air cooled below its dew point. Condensation occurs. Process follows constant WBT line approximately until ADP, then sensible cooling.
6.3 Cooling & Dehumidification Process
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Process: Air passes over cooling coil with surface temperature below air's dew point.
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Initial cooling (sensible) until dew point.
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Condensation starts → both sensible and latent heat removal → follows approx. constant WBT line.
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Final state depends on coil surface temperature.
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Apparatus Dew Point (ADP): Temperature of air leaving the coil if it were brought to saturation by contact with coil (theoretical exit condition).
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Bypass Factor (BF):
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Definition: Fraction of air that bypasses the coil without being affected.
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Formula:
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$$ BF = \frac{h_1 - h_2}{h_1 - h_{ADP}} = \frac{t_1 - t_2}{t_1 - t_{ADP}} \text{ (if constant } \omega \text{ process)} $$
Where:
* $$\displaystyle h_1, t_1 $$ = Inlet air enthalpy/DBT.
* $$\displaystyle h_2, t_2 $$ = **Actual** outlet air enthalpy/DBT.
* $$\displaystyle h_{ADP}, t_{ADP} $$ = Enthalpy/DBT of air at ADP (saturated at coil surface temp).
* **Significance:** Measures coil effectiveness. Lower BF = better coil performance. Affected by coil design, air velocity, fin spacing.
* **Outlet Conditions:** $$\displaystyle h_2 = h_1 - BF (h_1 - h_{ADP}) $$.
6.4 Air Mixing Problems
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Mass Balance (Dry Air): $$\displaystyle m_{a1} + m_{a2} = m_a $$
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Moisture Balance: $$\displaystyle m_{a1} \omega_1 + m_{a2} \omega_2 = m_a \omega $$
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Enthalpy Balance: $$\displaystyle m_{a1} h_1 + m_{a2} h_2 = m_a h $$
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Graphical Method: On psychrometric chart, join states 1 and 2. Mixed state lies on line connecting them. Distance ratio inversely proportional to mass flow rates.
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Fog Condition: If mixing line enters the two-phase region (inside dome), fog (visible moisture droplets) forms. Mixed state is on 100% RH line at same enthalpy as theoretical mix.
6.5 Summer Air Conditioning Load Calculations
- Sensible Heat Load ($$\displaystyle Q_s $$): Heat to be removed to lower DBT.
$$ Q_s = m_a C_{pa} (t_r - t_s) \quad \text{or} \quad Q_s = m_a (h_r - h_s)_{sensible} $$
- Latent Heat Load ($$\displaystyle Q_L $$): Heat to be removed to lower humidity.
$$ Q_L = m_a (\omega_r - \omega_s) h_{fg} \quad \text{or} \quad Q_L = m_a (h_r - h_s)_{latent} $$
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Total Heat Load ($$\displaystyle Q_T $$): $$\displaystyle Q_T = Q_s + Q_L = m_a (h_r - h_s) $$
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Sensible Heat Factor (SHF):
$$ \boxed{SHF = \frac{Q_s}{Q_T}} $$
* Ratio of sensible to total load. Determines slope of process line on psychrometric chart.
- Grand Sensible Heat Factor (GSHF): For multiple rooms/zoned systems. Overall SHF for entire plant.
$$ GSHF = \frac{\sum Q_s}{\sum Q_T} $$
- Factors for Summer Load: Solar radiation through walls/windows, occupants, lighting, equipment, infiltration, ventilation air.
[!TIP]
Critical Skill: Always use enthalpy difference ($$\displaystyle h_r - h_s $$) for total load and mass flow rate of dry air ($$\displaystyle m_a $$). SHF determines supply air state: from room condition, follow line with slope = SHF to saturation line (or to supply condition if over-cooling).
7.0 COMFORT & INDUSTRIAL AIR CONDITIONING
7.1 Comfort Air Conditioning
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Objective: Maintain indoor environment for human comfort and health.
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ASHRAE Comfort Zone: Defined by ranges of:
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Dry Bulb Temperature (typically 20-24°C summer, 20-24°C winter).
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Relative Humidity (typically 30-60%).
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Air Velocity (low, < 0.2 m/s).
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Mean Radiant Temperature (close to DBT).
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Clothing insulation and metabolic rate (activity level).
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Focus: Overall thermal comfort (PMV/PPD indices).
7.2 Industrial (Process) Air Conditioning
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Objective: Maintain environment for product/process requirements, not human comfort.
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Differences from Comfort AC:
| Comfort AC | Industrial/Process AC | | :--- | :--- | | Conditions for human comfort | Conditions for product quality, process yield, equipment operation. | | Moderate latent loads (from occupants) | Often high latent loads (from process moisture). | | Wider allowable ranges | Very strict temperature/humidity control (±1°C, ±5% RH). | | Focus on air quality (ventilation) | May require high air cleanliness (e.g., semiconductor, pharma). | | 24/7 operation typical | May have specific operating schedules. |
7.3 Design Conditions & Supply Air State
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Design Conditions: Specified indoor (room) DBT, RH, and outdoor design conditions.
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Supply Air State Determination:
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Plot room condition ($$\displaystyle t_r, \omega_r $$) on psychrometric chart.
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Calculate room sensible and latent loads → find SHF.
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From room condition, draw line with slope = SHF towards saturation line (or below if over-cooling).
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Intersection with saturation line gives Apparatus Dew Point (ADP).
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Supply air state ($$\displaystyle t_s, \omega_s $$) is located on this line such that $$\displaystyle m_a (h_r - h_s) = Q_T $$.
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If bypass factor (BF) is considered, actual supply state is between ADP and inlet state: $$\displaystyle h_s = h_1 - BF (h_1 - h_{ADP}) $$.
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8.0 SPECIAL REFRIGERATION SYSTEMS & APPLICATIONS
8.1 Steam Jet Refrigeration System
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Principle: Uses a high-pressure steam jet as the motive fluid. Steam expands through a nozzle, creating a vacuum in the evaporator. Low-pressure refrigerant (usually water) flashes/evaporates at low temperature, producing refrigeration.
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Components: Steam generator, steam nozzle, evaporator (at low pressure), condenser, condensate pump, ejector.
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Working (T-s/H-s Diagram):
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High-pressure steam (1) expands isentropically in nozzle to low pressure (2).
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Low pressure at nozzle exit induces refrigerant vapour from evaporator (3) and mixes.
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Mixture (4) is condensed in condenser.
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Condensate (5) pumped to evaporator pressure.
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Applications: Where cheap/waste steam is available (e.g., chemical plants, ice plants, ship refrigeration).
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Limitations: Low COP (typically 0.5-0.7), requires high-quality steam, large water flow rate.
8.2 Production of Dry Ice (Solid CO₂)
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Process:
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Liquid CO₂ is stored under pressure (≈ 20-25 bar) at ambient temperature.
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When released to atmospheric pressure through a nozzle or plate, it flash evaporates.
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Latent heat of vaporization is drawn from the remaining liquid, causing a portion to freeze into solid snow-like CO₂.
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This snow is compressed into blocks or pellets (dry ice).
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Key Point: Uses the Joule-Thomson effect (throttling) of CO₂ at its critical temperature region.
8.3 Applications of Refrigeration for Food Preservation
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Control of Microbial Growth: Low temperatures slow down or inhibit growth of bacteria, yeasts, molds.
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Control of Enzymatic Activity: Enzymes causing ripening, spoilage, texture change are slowed.
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Moisture Loss Prevention: Low temperature reduces evaporation from food, maintaining weight and quality.
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Other Applications: Ice making, cold storage (fruits, vegetables, meat, fish), refrigerated transport, display cabinets, food processing (freezing, chilling).
9.0 AUXILIARY & MAINTENANCE TOPICS
9.1 Leak Detection Methods
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Soap Solution: Apply to joints; bubbles indicate leak. Simple, for large leaks.
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Electronic Leak Detectors: Sniffing devices sensitive to refrigerant gases. Common for HFCs/HCFCs.
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UV Dye: Add dye to system; leaks show under UV light. Good for hard-to-find leaks.
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Halide Torch: Uses copper flame color change (green for CFCs/HCFCs). Obsolete due to toxicity/CFCs.
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Pressure Decay Test: Pressurize system with inert gas (N₂); monitor pressure drop over time.
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Ultrasonic: Detects sound of gas escaping.
9.2 By-Pass Factor of Cooling Coil
- Definition: Fraction of air that bypasses the coil without any change in state.
$$ BF = \frac{\text{Enthalpy difference (inlet to outlet)}}{\text{Enthalpy difference (inlet to ADP)}} $$
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Factors Affecting BF:
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Coil surface area (larger area → lower BF).
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Air velocity over coil (higher velocity → higher BF).
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Fin spacing and design.
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Number of rows.
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Significance: Determines actual outlet air condition. A coil with BF=0.2 means 20% of air is unaffected, 80% leaves at ADP.
9.3 Fog in Air
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Definition: Condition where air contains visible water droplets suspended. Occurs when air is supersaturated (RH > 100%) at a DBT above the dew point.
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Cause on Psychrometric Chart: When two air streams are mixed and the mixing line enters the two-phase region (inside the saturation dome). The mixture state is forced onto the 100% RH line (fog line) at the same enthalpy as the theoretical mix.
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Representation: Mixed state point lies on the saturation curve (100% RH line), even though DBT > original dew point of either stream.
[!TIP]
Exam Focus: Be able to identify fog condition on a psychrometric chart: mixing line crossing inside the dome → outlet on 100% RH line. Calculate using enthalpy balance and setting RH=100%.