Drag coefficient

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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

  1. Clancy, L.J. (1975). Aerodynamics. ISBN 0-273-01120-0.
  2. Abbott, Ira H., and Von Doenhoff, Albert E. (1959). Theory of Wing Sections.
  3. Hoerner, Dr. Sighard F., Fluid-Dynamic Drag.
  4. EngineeringToolbox.com - Drag Coefficient resources.
  5. NASA - Shape Effects on Drag.

Template:Aerospace engineering Template:Fluid dynamics