Carnot Heat Engine Efficiency Calculator
Carnot's Theorem establishes the Second-Law thermodynamic upper bound on thermal efficiency η for any heat engine operating between a hot source at absolute temperature T_H and cold sink at T_C.
Maximum theoretical work output per unit heat input (%)
Heat sink absolute temperature in Kelvin (27 °C = 300.15 K)
Heat source absolute temperature in Kelvin
Step-by-Step Calculation
Carnot's Theorem establishes the Second-Law thermodynamic upper bound on thermal efficiency η for any heat engine operating between a hot source at absolute temperature T_H and cold sink at T_C.
Real-World Reference Values
T_H ≈ 1,700 K firing temperature (~82% Carnot limit)
T_H ≈ 873 K (600 °C) steam conditions
Constrained by low T_H ≈ 420 K (150 °C) brine
20-Row Comparison Table
Carnot Thermal Efficiency (η (%)) · Cold Reservoir Temperature (K) (T_C (K))
| # | Cold Reservoir Temperature (K) (T_C (K)) | Carnot Thermal Efficiency (η (%)) | Δ % |
|---|---|---|---|
| 01 | 75.1125 | 90.6109 | +44.98% |
| 02 | 101.4151 | 87.3231 | +39.72% |
| 03 | 127.7178 | 84.0353 | +34.46% |
| 04 | 154.0204 | 80.7475 | +29.20% |
| 05 | 180.323 | 77.4596 | +23.94% |
| 06 | 206.6257 | 74.1718 | +18.67% |
| 07 | 232.9283 | 70.884 | +13.41% |
| 08 | 259.2309 | 67.5961 | +8.15% |
| 09 | 285.5336 | 64.3083 | +2.89% |
| 10 | 300 Current | 62.5 | 0.00% |
| 11 | 338.1388 | 57.7326 | -7.63% |
| 12 | 364.4414 | 54.4448 | -12.89% |
| 13 | 390.7441 | 51.157 | -18.15% |
| 14 | 417.0467 | 47.8692 | -23.41% |
| 15 | 443.3493 | 44.5813 | -28.67% |
| 16 | 469.652 | 41.2935 | -33.93% |
| 17 | 495.9546 | 38.0057 | -39.19% |
| 18 | 522.2572 | 34.7178 | -44.45% |
| 19 | 548.5599 | 31.43 | -49.71% |
| 20 | 574.8625 | 28.1422 | -54.97% |
Frequently Asked Questions
Why must T_C and T_H be in absolute Kelvin rather than Celsius?+
Thermodynamic entropy ratios (dQ/T) are defined strictly relative to absolute zero (0 K = -273.15 °C).
Why can no heat engine ever reach 100% Carnot efficiency?+
Achieving η = 100% would require either a cold sink at absolute zero (T_C = 0 K, forbidden by the Third Law) or an infinite hot source temperature.
Which improves efficiency faster: raising T_H by 50 K or lowering T_C by 50 K?+
Lowering the cold sink temperature T_C by ΔT always yields a larger percentage gain in Carnot efficiency than raising T_H by the same ΔT.