HVAC Systems Encyclopedia

A comprehensive encyclopedia of heating, ventilation, and air conditioning systems

Engine Coolant Heating Systems

Overview

Engine coolant heating systems recover waste heat from the internal combustion engine to provide cabin heating in automobiles. Unlike purpose-built heating systems, automotive coolant heating leverages the 60-75% of fuel energy that is rejected as waste heat through the cooling system, making it a highly efficient parasitic heat source. The system operates as a liquid-to-air heat exchanger network, transferring thermal energy from engine coolant (typically ethylene glycol/water mixture) to cabin air via the heater core.

Thermodynamic Principles

Waste Heat Recovery

Internal combustion engines convert only 25-35% of fuel chemical energy into mechanical work. The remainder is distributed between exhaust gas losses (30-40%) and coolant system heat rejection (30-35%). The coolant heat rejection rate can be calculated from:

$$Q_{reject} = \dot{m}{coolant} \cdot c_p \cdot (T{out} - T_{in})$$

where $\dot{m}{coolant}$ is the coolant mass flow rate (typically 0.5-2.0 kg/s), $c_p$ is the specific heat of the coolant mixture (approximately 3.5 kJ/kg·K for 50/50 ethylene glycol/water), $T{out}$ is the engine outlet temperature (85-105°C), and $T_{in}$ is the return temperature (75-90°C).

For a typical 2.0L engine at 3000 RPM producing 50 kW of mechanical power, the coolant heat rejection is approximately 20-30 kW, far exceeding typical cabin heating loads of 3-6 kW at moderate outdoor temperatures.

Coolant-to-Air Heat Transfer

The heater core functions as a crossflow heat exchanger with coolant flowing through tubes and air passing over finned surfaces. The heat transfer rate is governed by:

$$Q = UA \cdot LMTD$$

where $U$ is the overall heat transfer coefficient (typically 200-400 W/m²·K for automotive heater cores), $A$ is the heat transfer surface area (0.5-1.5 m² for passenger vehicles), and $LMTD$ is the logarithmic mean temperature difference:

$$LMTD = \frac{(T_{c,in} - T_{a,out}) - (T_{c,out} - T_{a,in})}{\ln\left(\frac{T_{c,in} - T_{a,out}}{T_{c,out} - T_{a,in}}\right)}$$

System Components and Control

Thermostat Operation

The coolant thermostat serves dual purposes: maintaining optimal engine temperature (typically 85-95°C per SAE J2534) and regulating heat availability for cabin heating. Wax-pellet thermostats operate on thermal expansion principles:

graph TD
    A[Cold Engine Start] --> B{Coolant Temp < 85°C?}
    B -->|Yes| C[Thermostat Closed]
    C --> D[Coolant Bypasses Radiator]
    D --> E[Rapid Warmup]
    E --> B
    B -->|No| F[Thermostat Opens]
    F --> G[Coolant Flows to Radiator]
    G --> H[Temperature Regulation]
    H --> I{Temp Drops?}
    I -->|Yes| B
    I -->|No| H

The thermostat opening temperature affects cabin heating performance. A higher setpoint (90-95°C) provides greater heating capacity but may increase warm-up time by 15-25% compared to an 82-88°C thermostat.

Coolant Flow Control

Coolant circulation is driven by either mechanical water pumps (belt-driven) or electric pumps in modern vehicles. Flow rate control strategies include:

Control MethodFlow RegulationAdvantagesDisadvantages
Fixed Mechanical PumpNone (speed proportional to engine RPM)Simple, reliableOvercooling at idle, parasitic losses
Variable Speed Electric PumpPWM control 0-100%Optimized flow, reduced power consumptionAdded electrical load, complexity
Dual-Speed MechanicalClutch engagementImproved low-speed performanceLimited control resolution

Electric pumps provide precise flow control with typical power consumption of 50-150W, enabling coolant circulation during engine-off operation for auxiliary heaters or electric vehicles.

Heater Core Sizing

Heater core capacity must satisfy peak heating demand while minimizing pressure drop and packaging volume. Sizing calculations follow:

$$Q_{required} = \dot{m}{air} \cdot c{p,air} \cdot (T_{discharge} - T_{ambient})$$

For a mid-size sedan requiring 50 g/s airflow at 45°C discharge temperature in -20°C conditions:

$$Q_{required} = 0.05 \times 1.006 \times (45 - (-20)) = 3.27 \text{ kW}$$

With coolant inlet temperature of 90°C and a design outlet of 70°C (20°C drop), the required coolant flow rate is:

$$\dot{m}{coolant} = \frac{Q{required}}{c_p \cdot \Delta T} = \frac{3270}{3500 \times 20} = 0.047 \text{ kg/s}$$

Warmup Time Analysis

Cold start warmup time critically affects passenger comfort and defrosting performance. The warmup transient can be modeled as:

$$M_{coolant} \cdot c_p \cdot \frac{dT}{dt} = Q_{combustion} - Q_{radiator} - Q_{heatercore} - Q_{losses}$$

where $M_{coolant}$ is the total coolant mass (4-8 kg typical). For a simplified case with thermostat closed (no radiator flow) and heater core off:

$$t_{warmup} = \frac{M_{coolant} \cdot c_p \cdot \Delta T}{P_{engine} \cdot \eta_{heating}}$$

For a 5 kg coolant system warming from 0°C to 85°C with a 30 kW engine at 40% heating efficiency:

$$t_{warmup} = \frac{5 \times 3500 \times 85}{30000 \times 0.4} = 124 \text{ seconds} \approx 2.1 \text{ minutes}$$

Actual warmup times extend to 5-10 minutes due to cabin heating loads, radiator losses, and variable engine power during driving.

Auxiliary Heating Systems

Modern vehicles employ auxiliary heaters to reduce cold-start discomfort:

graph LR
    A[Fuel Tank] --> B[Auxiliary Heater<br/>Webasto/Eberspacher]
    B --> C[Coolant Loop]
    C --> D[Heater Core]
    D --> E[Cabin Air]
    C --> F[Engine Block]
    G[Battery] --> B

Auxiliary fuel-fired heaters (per SAE J2757) provide 2-5 kW heating capacity independent of engine operation, consuming 0.2-0.5 L/hr of fuel. These systems pre-warm the coolant loop, reducing warmup time by 50-70% and improving cold-start emissions.

Performance Considerations

Coolant-to-air heating effectiveness depends on multiple factors:

  • Coolant temperature: Each 10°C increase in coolant temperature yields approximately 15-20% increase in heating capacity at constant airflow
  • Airflow rate: Heating capacity increases nearly linearly with airflow up to the point where air-side thermal resistance dominates
  • Altitude effects: Reduced air density at altitude decreases mass flow rate by approximately 3% per 1000 ft elevation
  • Glycol concentration: Higher glycol content (>50%) reduces specific heat and thermal conductivity, decreasing heat transfer by 5-10%

Standards and Testing

SAE J2765 defines test procedures for automotive HVAC systems, including:

  • Steady-state heating capacity measurement at -18°C, 0°C, and 20°C ambient
  • Transient warmup performance from cold start
  • Coolant flow rate and pressure drop characterization
  • Heater core effectiveness rating