❄ Thermodynamics · Everyday Science
📅 Березень 2026⏱ 11 min🟡 Середній

How Refrigerators Work: The Thermodynamics of Cooling

A refrigerator doesn't create cold — it moves heat from inside the fridge to the outside. This is thermodynamically "unnatural" (heat spontaneously flows from hot to cold, not the reverse), so it requires work — typically 100–200 W of electrical power. The same principle drives air conditioners, heat pumps, and industrial chillers.

1. The Second Law & Why Cooling Costs Work

The second law of thermodynamics states that heat spontaneously flows from hot to cold, never the reverse. A refrigerator moves heat from a cold space (5°C) to a warm space (room at 25°C) — against the natural direction. This requires external work input.

Clausius statement of the 2nd law: "No process is possible whose sole result is the transfer of heat from a cooler body to a hotter body." Refrigerator energy balance: Q_hot = Q_cold + W Q_cold = heat removed from fridge interior W = electrical work input (compressor) Q_hot = heat rejected to kitchen (Q_cold + W) Your fridge heats your kitchen more than it cools its interior!

2. The Vapour-Compression Cycle

Nearly every domestic refrigerator, air conditioner, and heat pump uses the vapour-compression cycle. It exploits the fact that a fluid absorbs large amounts of heat when it evaporates (latent heat) and releases that heat when it condenses.

1Compression

Compressor pressurises the low-pressure vapour → high-pressure hot vapour (60–70°C)

2Condensation

Hot vapour flows through condenser coils (back of fridge). Heat escapes to room air. Vapour condenses to high-pressure liquid.

3Expansion

Liquid passes through expansion valve (capillary tube). Pressure drops sharply → temperature drops to −20 to −30°C.

4Evaporation

Cold liquid flows through evaporator coils (inside fridge). Absorbs heat from food. Liquid evaporates to low-pressure vapour. Returns to compressor.

3. The Four Components

4. COP & Carnot Limit

Coefficient of Performance (refrigerator): COP_cold = Q_cold / W = "cooling obtained per unit work" Carnot (ideal reversible) limit: COP_Carnot = T_cold / (T_hot − T_cold) Example: fridge at 5°C (278 K), room at 25°C (298 K) COP_Carnot = 278 / (298 − 278) = 278 / 20 = 13.9 Real domestic fridges: COP ≈ 2–5 (15–35% of Carnot ideal) For a freezer at −18°C (255 K), room at 25°C (298 K): COP_Carnot = 255 / 43 = 5.9 Real: COP ≈ 1.5–2.5 → Freezers are inherently less efficient than fridges (larger temperature difference)

A COP of 3 means for every 1 W of electricity, 3 W of heat is removed from the fridge — and 4 W is dumped into the kitchen (Q_cold + W). Higher COP = better efficiency. The EU energy label rates fridges from A (best, COP ~4+) to G (worst).

5. Refrigerants: From CFCs to R-290

GenerationTypeExampleODPGWPStatus
1930s–1990sCFCR-12 (Freon)1.010,900Banned (Montreal 1987)
1990s–2020sHCFCR-220.0551,810Phased out (2020–2030)
2000s–presentHFCR-134a01,430Being phased down (Kigali 2016)
ModernHFOR-1234yf04Automotive AC replacement
ModernHydrocarbonR-290 (propane)03Domestic fridges (EU standard)
ModernNaturalR-744 (CO₂)01Commercial/heat pumps

ODP = Ozone Depletion Potential (relative to R-11). GWP = Global Warming Potential over 100 years (relative to CO₂). The shift is toward natural refrigerants (propane, CO₂, ammonia) with near-zero GWP. R-290 (propane) is now used in ~50% of new European domestic refrigerators — flammable but safe in the small charges used (~57 g).

6. Heat Pumps: Refrigeration in Reverse

A heat pump is the same vapour-compression cycle, but the useful output is the heat rejected (Q_hot) rather than the cooling (Q_cold). It pumps heat from outside air (even at 0°C) into a building.

Heat pump COP: COP_hot = Q_hot / W = (Q_cold + W) / W = COP_cold + 1 Example: outdoor 0°C (273 K), indoor 20°C (293 K) COP_Carnot,hot = T_hot / (T_hot − T_cold) = 293 / 20 = 14.7 Real heat pump: COP ≈ 3–5 A COP of 4 means: for every 1 kWh of electricity, 4 kWh of heat is delivered to the building Compared to: Gas boiler: ~0.9 kWh heat per 1 kWh gas Electric resistance heater: ~1.0 kWh heat per 1 kWh electricity Heat pump: ~3–4 kWh heat per 1 kWh electricity → Heat pumps are 3–4× more efficient than direct electric heating

Air-source heat pumps work well down to about −15°C. Below that, COP drops significantly and supplementary heating may be needed. Ground-source heat pumps (using underground loops at ~10°C year-round) maintain higher COP but are more expensive to install.

7. Alternative Cooling Technologies

Global cooling demand: Air conditioning uses ~10% of global electricity and is growing fast — the number of AC units worldwide is projected to triple from 2 billion (2024) to 5.6 billion by 2050. Improving COP by even 10% would save more electricity than many countries consume.