Ideal cycle for gasoline engines, assuming constant-volume combustion.
Theoretical efficiency is higher than the practical 30–35% of real engines.
Visualize Carnot, Otto, Diesel, and Brayton cycles on P-V and T-s diagrams in real time. Instantly compute thermal efficiency, net work, and heat exchange quantities.
$$\eta_\text{Carnot} = 1 - \frac{T_L}{T_H}$$
The highest efficiency achievable by any reversible cycle operating between the same two temperature reservoirs.
$$\eta_\text{Otto} = 1 - \frac{1}{r_c^{\,\gamma-1}}$$
Determined by compression ratio $r_c = V_1/V_2$. Example: $r_c=9, \gamma=1.4$ → η ≈ 58%
$$\eta_\text{Diesel} = 1 - \frac{1}{r_c^{\gamma-1}}\cdot\frac{r_\text{CO}^\gamma - 1}{\gamma(r_\text{CO}-1)}$$
Characterized by high compression ratio and constant-pressure combustion.
$$\eta_\text{Brayton} = 1 - r_p^{\,(1-\gamma)/\gamma}$$
Determined by pressure ratio $r_p$. The fundamental cycle for gas turbines and jet engines.