For subsonic and transonic aircraft below critical Mach number, total drag coefficient ($C_D$) is expressed as the parabolic drag polar:
The Subsonic Drag Polar Equation:
$$C_D = C_{D0} + C_{Di} = C_{D0} + k C_L^2 = C_{D0} + \frac{C_L^2}{\pi e \text{AR}}$$
The Golden Condition for Maximum Aerodynamic Efficiency $(L/D)_{\max}$
The overall aerodynamic efficiency of an aircraft is measured by its lift-to-drag ratio:
$$\frac{L}{D} = \frac{C_L}{C_D} = \frac{C_L}{C_{D0} + k C_L^2}$$
To find the condition where $(L/D)$ is maximized, we differentiate $(C_D/C_L)$ with respect to $C_L$ and equate to zero:
$$\frac{d}{d C_L}\left(\frac{C_{D0} + k C_L^2}{C_L}\right) = -\frac{C_{D0}}{C_L^2} + k = 0 \implies C_{D0} = k C_L^2 = C_{Di}$$
Worked Numerical 2: Drag Polar Analysis (UPSC Pattern)
Problem: A commuter transport has a wing aspect ratio $\text{AR} = 9.0$, Oswald efficiency factor $e = 0.85$, and zero-lift parasite drag coefficient $C_{D0} = 0.024$. Calculate: (1) The induced drag factor $k$, (2) The lift coefficient for maximum $L/D$, and (3) The maximum lift-to-drag ratio $(L/D)_{\max}$.
Solution:
- Compute induced drag factor $k$:
$$k = \frac{1}{\pi e \text{AR}} = \frac{1}{\pi \times 0.85 \times 9.0} = \frac{1}{24.033} \approx 0.0416$$
- Compute $C_L$ at maximum $L/D$:
$$C_{L,\text{md}} = \sqrt{\frac{C_{D0}}{k}} = \sqrt{\frac{0.024}{0.0416}} = \sqrt{0.5769} \approx 0.760$$
- Compute $(L/D)_{\max}$:
$$\left(\frac{L}{D}\right)_{\max} = \frac{C_{L,\text{md}}}{2 C_{D0}} = \frac{0.760}{2 \times 0.024} = \frac{0.760}{0.048} \approx 15.83$$
Conclusion: The aircraft achieves its best aerodynamic glide efficiency of $15.83:1$ when trimmed to $C_L = 0.760$.