Evaporator Performance Analysis
Performance Fundamentals
Evaporator performance determines refrigeration system capacity, efficiency, and operating economics. Performance analysis requires understanding heat transfer mechanisms, refrigerant-side and load-side characteristics, and degradation factors affecting long-term operation.
The evaporator transfers heat from the cooling medium (air, water, or process fluid) to the evaporating refrigerant. Performance depends on:
- Heat transfer surface area and geometry
- Temperature difference between load and refrigerant
- Flow characteristics on both sides
- Surface conditions and cleanliness
- Refrigerant distribution quality
Heat Transfer Analysis Methods
Log Mean Temperature Difference (LMTD) Method
The LMTD method applies to evaporators with known inlet and outlet temperatures. For constant evaporating temperature (typical for direct expansion systems):
Heat Transfer Equation:
Q = U × A × LMTD
Where:
- Q = Heat transfer rate (Btu/hr or kW)
- U = Overall heat transfer coefficient (Btu/hr·ft²·°F or W/m²·K)
- A = Heat transfer surface area (ft² or m²)
- LMTD = Log mean temperature difference (°F or K)
LMTD Calculation for Constant Evaporating Temperature:
LMTD = (ΔT₁ - ΔT₂) / ln(ΔT₁/ΔT₂)
Where:
- ΔT₁ = Load inlet temperature - Evaporating temperature
- ΔT₂ = Load outlet temperature - Evaporating temperature
For air-cooling evaporators with significant temperature change, account for sensible and latent heat components separately.
Effectiveness-NTU Method
The effectiveness-NTU method applies when outlet temperatures are unknown, particularly useful for design calculations and performance prediction.
Heat Transfer Effectiveness:
ε = Q_actual / Q_maximum
Q_maximum = C_min × (T_load,in - T_evap)
Where:
- ε = Heat exchanger effectiveness (dimensionless)
- C_min = Minimum heat capacity rate (Btu/hr·°F or W/K)
- T_load,in = Load fluid inlet temperature
- T_evap = Evaporating temperature
Number of Transfer Units (NTU):
NTU = U × A / C_min
For evaporators with constant evaporating temperature (C_refrigerant approaches infinity):
ε = 1 - exp(-NTU)
This relationship simplifies performance prediction when overall heat transfer coefficient and surface area are known.
Comparison of Methods
| Method | Best Application | Advantages | Limitations |
|---|---|---|---|
| LMTD | Performance verification, known temperatures | Simple, direct calculation | Requires all temperatures known |
| Effectiveness-NTU | Design calculations, rating | Works with unknown outlet conditions | More complex relationships |
| Hybrid approach | Complex geometries | Combines benefits of both | Requires careful application |
Overall Heat Transfer Coefficient
The overall heat transfer coefficient combines thermal resistances in series:
1/U = 1/h_outside + t_wall/k_wall + R_fouling,outside + R_fouling,inside + 1/h_inside
Where:
- h_outside = Load-side convective coefficient
- h_inside = Refrigerant-side convective coefficient
- t_wall = Tube wall thickness
- k_wall = Tube material thermal conductivity
- R_fouling = Fouling resistance factors
Typical Heat Transfer Coefficients
| Evaporator Type | Load Medium | U-Value Range (Btu/hr·ft²·°F) | U-Value Range (W/m²·K) |
|---|---|---|---|
| DX air coil | Air | 15-30 | 85-170 |
| Flooded shell-and-tube | Water | 150-300 | 850-1700 |
| DX shell-and-tube | Water | 100-200 | 570-1135 |
| Plate heat exchanger | Water/glycol | 200-500 | 1135-2840 |
| Flooded evaporator | Brine | 120-250 | 680-1420 |
Values represent clean conditions. Fouling reduces U significantly.
Approach Temperature Analysis
Approach temperature represents the temperature difference between load fluid outlet and refrigerant evaporating temperature. It indicates heat transfer effectiveness.
Approach Temperature:
TD_approach = T_load,out - T_evap
Lower approach temperatures indicate:
- Larger heat transfer surface area
- Better heat transfer characteristics
- Higher evaporating temperature for given load
- Improved system efficiency
Approach Temperature Optimization
Optimum approach temperature balances capital cost against operating cost:
Economic Analysis:
- Smaller approach → Larger evaporator → Higher first cost
- Smaller approach → Higher evaporating temperature → Lower compressor power
- Optimal design minimizes life cycle cost
| Application | Typical Approach (°F) | Typical Approach (K) | Design Consideration |
|---|---|---|---|
| Chilled water | 3-5 | 1.7-2.8 | Balance size vs. efficiency |
| Process cooling | 5-10 | 2.8-5.6 | Process requirements dictate |
| Air conditioning | 8-15 | 4.4-8.3 | Coil size constraints |
| Low-temperature | 5-8 | 2.8-4.4 | Moisture concerns |
| Ice building | 3-5 | 1.7-2.8 | Ice formation rate critical |
Impact on System Performance
Each 1°F (0.56K) reduction in approach temperature:
- Increases evaporating temperature by approximately 1°F
- Reduces compressor power by 2-4% (varies with refrigerant and conditions)
- Requires 10-15% more evaporator surface area
- Reduces refrigerant-side pressure drop concerns
Fouling Effects on Performance
Fouling adds thermal resistance, reducing heat transfer and increasing approach temperature. Fouling occurs on load side and refrigerant side.
Load-Side Fouling
Air-Side Fouling:
- Dust and particulate accumulation
- Biological growth (mold, bacteria)
- Corrosion products
- Increases air-side resistance dramatically
Water-Side Fouling:
- Scale formation (calcium carbonate, magnesium silicate)
- Biological fouling (algae, biofilm)
- Corrosion products (iron oxide, copper oxide)
- Particulate deposition
Fouling Resistance Values
| Fouling Source | Clean Condition | Fouled Condition | Typical Fouling Factor |
|---|---|---|---|
| Filtered air | R = 0 | Add 0.0005-0.002 hr·ft²·°F/Btu | 25-40% capacity loss |
| Cooling tower water | 0.001 | 0.003-0.005 hr·ft²·°F/Btu | Add 0.002-0.004 |
| Closed loop water | 0.0005 | 0.001-0.002 hr·ft²·°F/Btu | Add 0.0005-0.0015 |
| Glycol solution | 0.001 | 0.002-0.003 hr·ft²·°F/Btu | Add 0.001-0.002 |
| River/lake water | 0.002 | 0.005-0.008 hr·ft²·°F/Btu | Add 0.003-0.006 |
Convert to SI: 1 hr·ft²·°F/Btu = 0.1761 m²·K/W
Refrigerant-Side Fouling
Less common but critical when present:
- Oil accumulation (reduces heat transfer coefficient by 10-30%)
- Non-condensable gases (reduce effective surface area)
- Contaminants from system degradation
- Refrigerant decomposition products
Oil Effect on Heat Transfer:
For 5% oil concentration in evaporator:
- Heat transfer coefficient reduction: 15-25%
- Greater impact at low evaporating temperatures
- Flooded evaporators more susceptible than DX
Performance Degradation Factors
Frost Formation Effects
Frost accumulation on air-cooling evaporators creates multiple performance penalties:
Thermal Resistance:
- Frost adds insulating layer
- Thermal conductivity of frost: 0.12-0.25 Btu/hr·ft·°F (0.21-0.43 W/m·K)
- Reduces effective U-value by 20-60%
Airflow Restriction:
- Frost blocks airflow passages
- Increases air-side pressure drop exponentially
- Reduces airflow by 30-70% before defrost
- Non-uniform frost distribution causes air bypass
Frost Density Impact:
| Operating Condition | Frost Density (lb/ft³) | Thermal Conductivity | Growth Rate |
|---|---|---|---|
| High humidity, -10°F | 6-12 | Low | Very rapid |
| Medium humidity, 0°F | 12-20 | Medium | Moderate |
| Low humidity, 20°F | 20-30 | Higher | Slow |
Frost density increases with time as consolidation occurs.
Refrigerant Maldistribution
Poor refrigerant distribution reduces effective surface area utilization:
Impact Factors:
- Overfed circuits: liquid carryover, reduced superheat control
- Underfed circuits: reduced capacity, excessive superheat
- Combined effect: 10-40% capacity loss possible
Distribution Quality Metric:
Circuit efficiency = (Actual capacity) / (Capacity if perfectly distributed) × 100%
Well-designed systems achieve 85-95% distribution efficiency.
Air or Water Flow Variation
Flow rate changes affect heat transfer coefficients non-linearly:
Air-Side Relationship (Turbulent Flow):
h ∝ V^0.8
Where V = air velocity
Reducing airflow by 20% reduces heat transfer coefficient by approximately 17%.
Water-Side Relationship (Turbulent Flow):
h ∝ V^0.8
Similar relationship, but water-side typically has lower thermal resistance.
Defrost System Performance
Defrost Methods and Efficiency
| Defrost Method | Energy Source | Efficiency | Typical Duration | Application |
|---|---|---|---|---|
| Hot gas | Compressor discharge | 60-75% | 15-30 minutes | Most commercial systems |
| Electric | Resistance heaters | 95-100% | 20-45 minutes | Small units, freezers |
| Water | Warm water spray | 70-85% | 10-20 minutes | Marine, fish processing |
| Reverse cycle | Heat pump reversal | 65-80% | 20-40 minutes | Heat pumps only |
| Off-cycle | Room air | 0% added | 45-90 minutes | Above 35°F applications |
Hot Gas Defrost
Most common method for commercial refrigeration:
Process Sequence:
- Liquid line solenoid closes
- Hot gas valve opens
- Evaporator fans stop (typically)
- Hot refrigerant vapor enters evaporator
- Frost melts from inside out
- Termination by time or temperature
Performance Considerations:
- Requires 15-25% of system capacity during defrost
- Heat input: 12,000-18,000 Btu/hr per ton of evaporator capacity
- Refrigerant charge increases during defrost (receiver sizing critical)
- Multiple evaporators require sequenced defrost
Electric Defrost
Heater Sizing:
kW = (Evaporator capacity in tons × 12,000 × 1.5) / 3413
Factor 1.5 accounts for:
- Melting ice (144 Btu/lb at 32°F)
- Heating coil mass
- Heat losses
- Safety margin
Energy Impact:
Electric defrost typically adds 5-15% to total system energy consumption depending on:
- Defrost frequency (cycles per day)
- Duration per cycle
- Operating temperature
- Humidity conditions
Performance Monitoring and Maintenance
Key Performance Indicators
| Parameter | Measurement | Normal Range | Action Required |
|---|---|---|---|
| Approach temperature | T_load,out - T_evap | Design ± 2°F | >5°F deviation: clean/inspect |
| Superheat | T_suction - T_evap | 8-12°F DX, 4-6°F flooded | Adjust TXV/check distribution |
| Air-side pressure drop | ΔP across coil | Design ± 20% | >40% increase: clean coil |
| Water-side pressure drop | ΔP through exchanger | Design ± 25% | >50% increase: chemical clean |
| Capacity ratio | Actual/Design capacity | 95-105% | <90%: investigate degradation |
Maintenance Impact on Performance
Regular maintenance preserves design performance:
Air-Side Cleaning:
- Coil cleaning restores 80-95% of original capacity
- Frequency: 2-4 times per year (varies by environment)
- Methods: vacuum, compressed air, chemical wash, steam
Water-Side Cleaning:
- Chemical cleaning restores 85-100% of original capacity
- Frequency: annually or per water analysis
- Methods: acid cleaning, mechanical brushing (tube bundles)
Refrigerant Charge Optimization:
- Proper charge within ±5% of design
- Undercharge reduces capacity proportionally
- Overcharge in DX systems causes hunting, liquid slugging
Performance Testing and Verification
Field Performance Test Procedure:
- Stabilize system at design conditions (minimum 30 minutes)
- Measure refrigerant saturation temperature (evaporating temperature)
- Measure load-side inlet and outlet temperatures
- Measure load-side flow rate
- Calculate heat transfer rate: Q = m × cp × ΔT
- Calculate approach temperature
- Compare to design values
- Determine U-value and compare to clean design condition
Acceptance Criteria:
- Capacity within ±5% of design
- Approach temperature within ±2°F of design
- U-value within 10% of clean design (new installation)
- U-value within 25% of clean design (existing system)
Advanced Performance Considerations
Variable Load Operation
Part-load performance differs from design conditions:
- Reduced load → lower temperature difference → reduced LMTD
- May require capacity control (VFD fans, water flow modulation)
- Flooded systems maintain better part-load performance than DX
- Minimum loading: typically 25-40% of design capacity
Low-Temperature Applications
Below 0°F evaporating temperature:
- Frost formation accelerates dramatically
- Defrost frequency increases (4-12 cycles per day)
- Approach temperature typically larger (6-10°F)
- Material selection critical (brittle fracture concerns)
- Oil return becomes challenging
High-Efficiency Design Strategies
Maximize performance through:
- Oversized surface area (reduce approach by 30-50%)
- Enhanced surfaces (microfin tubes, louvered fins)
- Optimized circuitry (minimize refrigerant-side pressure drop)
- Superior distribution (multiple feedpoints, distributors)
- Variable-speed fans (maintain optimum air velocity)
- Water treatment programs (minimize fouling)
- Advanced defrost controls (demand-based, not time-based)
ROI Analysis:
High-efficiency evaporator design typically adds 15-25% to evaporator cost but:
- Reduces annual energy cost by 8-15%
- Simple payback: 2-5 years (varies with utility rates)
- Extended equipment life through reduced compressor stress
- Improved process control and product quality
Performance Optimization Summary
Optimal evaporator performance requires:
- Proper initial sizing with appropriate approach temperature
- High-quality refrigerant distribution system
- Regular maintenance program (cleaning, refrigerant charge)
- Advanced controls for demand-based defrost
- Performance monitoring and trending
- Water treatment for water-cooled applications
- Adequate air filtration for air-cooled applications
Performance degradation is gradual and often unnoticed. Establish baseline performance at commissioning and monitor quarterly. A 20% capacity loss typically occurs over 2-3 years without proper maintenance, directly impacting system efficiency and operating cost.