12.10 Refrigerator & Heat Pump Visualizer

Refrigerators and Heat Pumps

Refrigerators and Heat Pumps

Thermodynamic Cycle Visualization

Hot Reservoir (T₁ = 300K) Cold Reservoir (T₂ = 275K) Working Substance (Refrigerant Cycle) Q₁ = 500J Q₂ = 400J W = 100J α = 4.0 Coefficient of Performance

This enhanced diagram illustrates the thermodynamic cycle of refrigeration systems. The working substance extracts heat Q₂ (400J) from the cold reservoir, external work W (100J) is performed on the system, and heat Q₁ (500J) is rejected to the hot reservoir. The coefficient of performance (α) for this example is 4.0.

Coefficient of Performance (α) = Q₂/W = 400J/100J = 4.0

Refrigerator Operation

Designed to maintain a space at low temperature by continuously removing heat from it.

  • Expansion: Refrigerant expands through a valve, cooling dramatically
  • Evaporation: Cold liquid absorbs heat (Q₂) from refrigerated space
  • Compression: Vapor is compressed, increasing temperature/pressure
  • Condensation: Hot gas releases heat (Q₁) to surroundings
  • Q₁ = Q₂ + W (First Law of Thermodynamics)

    Heat Pump Operation

    Uses the same cycle to transfer heat into a space for heating purposes.

  • Outdoor Coil: Extracts heat (Q₂) from outside air (even when cold)
  • Compression: Work (W) input increases refrigerant temperature
  • Indoor Coil: Releases high-grade heat (Q₁) to interior space
  • Expansion: Pressure reduction prepares for next cycle
  • Heating COP = Q₁/W = 500J/100J = 5.0

    More efficient than resistive heating (COP=1.0)

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