Drag coefficient
Drag Coefficient (commonly denoted as: c_d, c_x, or c_w) is a dimensionless quantity used to quantify the drag or resistance of an object in a fluid environment, such as air or water. It indicates how aerodynamic or hydrodynamic a body is. A lower drag coefficient corresponds to lower aerodynamic drag for a given shape.
Definition
The drag coefficient c_d is defined as:
c_d = (2 * F_d) / (ρ * u² * A)
where:
- F_d is the drag force.
- ρ is the mass density of the fluid.
- u is the flow velocity relative to the fluid.
- A is the reference area (e.g., frontal area for cars, wing area for aircraft).
Key Points
- The reference area depends on the object and context.
- Airfoils use wing area; cars use projected frontal area.
- For streamlined bodies (e.g., fish, aircraft), c_d is typically lower.
- For bluff bodies (e.g., brick, sphere), c_d is higher due to flow separation and pressure drag.
Cauchy Momentum Equation
In terms of local shear stress τ and local dynamic pressure q:
c_d = τ / q = (2 * τ) / (ρ * u²)
where:
- τ is the local shear stress.
- q is the dynamic pressure (q = 0.5 * ρ * u²).
Drag Equation
The general drag force formula:
F_d = 0.5 * ρ * u² * c_d * A
Dependence on Reynolds Number
The drag coefficient is influenced by the Reynolds number (Re):
- Low Re: laminar flow, drag dominated by viscous forces.
- High Re: turbulent flow, drag dominated by pressure forces.
- For a sphere: c_d drops sharply at the critical Reynolds number.
Drag Coefficient Examples
General Shapes
| Shape | c_d |
|---|---|
| Smooth sphere (Re = 10⁶) | 0.1 |
| Rough sphere (Re = 10⁶) | 0.47 |
| Flat plate perpendicular to flow (3D) | 1.28 |
| Empire State Building | 1.3–1.5 |
| Eiffel Tower | 1.8–2.0 |
| Long flat plate perpendicular to flow (2D) | 1.98–2.05 |
Aircraft
| Aircraft Type | c_d | Drag Count |
|---|---|---|
| F-4 Phantom II (subsonic) | 0.021 | 210 |
| Learjet 24 | 0.022 | 220 |
| Boeing 787 | 0.024 | 240 |
| Airbus A380 | 0.0265 | 265 |
| Cessna 172/182 | 0.027 | 270 |
| Boeing 747 | 0.031 | 310 |
| F-104 Starfighter | 0.048 | 480 |
Blunt and Streamlined Body Flows
- Streamlined bodies: Flow remains attached longer; friction drag dominates.
- Blunt bodies: Flow separates early; pressure drag dominates.
Boundary layer behavior is critical:
- Laminar flow = lower drag
- Turbulent flow = higher drag but more stable separation.
Drag Crisis
At critical Reynolds numbers, c_d can drop dramatically due to a transition to turbulent boundary layer flow (e.g., golf ball dimples reduce c_d).
See Also
References
- Clancy, L.J. (1975). Aerodynamics. ISBN 0-273-01120-0.
- Abbott, Ira H., and Von Doenhoff, Albert E. (1959). Theory of Wing Sections.
- Hoerner, Dr. Sighard F., Fluid-Dynamic Drag.
- EngineeringToolbox.com - Drag Coefficient resources.
- NASA - Shape Effects on Drag.