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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.
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'''Drag Coefficient''' (commonly denoted as: <math>c_d</math>, <math>c_x</math>, or <math>c_w</math>) 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 ==
== Definition ==
The drag coefficient \( c_d \) is defined as:
The drag coefficient <math>c_d</math> is defined as:


\[ c_d = \frac{2F_d}{\rho u^2 A} \]
<math>c_d = \frac{2F_d}{\rho u^2 A}</math>


where:
where:
* \( F_d \) is the drag force.
* <math>F_d</math> is the drag force.
* \( \rho \) is the mass density of the fluid.
* <math>\rho</math> is the mass density of the fluid.
* \( u \) is the flow velocity relative to the fluid.
* <math>u</math> is the flow velocity relative to the fluid.
* \( A \) is the reference area (e.g., frontal area for cars, wing area for aircraft).
* <math>A</math> is the reference area (e.g., frontal area for cars, wing area for aircraft).


== Key Points ==
== Key Points ==
* The reference area depends on the object and context.
* The reference area depends on the object and context.
* Airfoils use wing area; cars use projected frontal area.
* Airfoils use wing area; cars use projected frontal area.
* For streamlined bodies (e.g., fish, aircraft), \( c_d \) is typically lower.
* For streamlined bodies (e.g., fish, aircraft), <math>c_d</math> is typically lower.
* For bluff bodies (e.g., brick, sphere), \( c_d \) is higher due to flow separation and pressure drag.
* For bluff bodies (e.g., brick, sphere), <math>c_d</math> is higher due to flow separation and pressure drag.


== Cauchy Momentum Equation ==
== Cauchy Momentum Equation ==
In terms of local shear stress \( \tau \) and local dynamic pressure \( q \):
In terms of local shear stress <math>\tau</math> and local dynamic pressure <math>q</math>:


\[ c_d = \frac{\tau}{q} = \frac{2\tau}{\rho u^2} \]
<math>c_d = \frac{\tau}{q} = \frac{2\tau}{\rho u^2}</math>


where:
where:
* \( \tau \) = local shear stress.
* <math>\tau</math> = local shear stress.
* \( q \) = \( \frac{1}{2} \rho u^2 \), the dynamic pressure.
* <math>q = \frac{1}{2} \rho u^2</math>, the dynamic pressure.


== Drag Equation ==
== Drag Equation ==
The general drag force formula:
The general drag force formula:


\[ F_d = \frac{1}{2} \rho u^2 c_d A \]
<math>F_d = \frac{1}{2} \rho u^2 c_d A</math>


== Dependence on Reynolds Number ==
== Dependence on Reynolds Number ==
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* Low Re: laminar flow, drag dominated by viscous forces.
* Low Re: laminar flow, drag dominated by viscous forces.
* High Re: turbulent flow, drag dominated by pressure forces.
* High Re: turbulent flow, drag dominated by pressure forces.
* For a sphere: \( c_d \) drops sharply at the critical Reynolds number.
* For a sphere: <math>c_d</math> drops sharply at the critical Reynolds number.


== Drag Coefficient Examples ==
== Drag Coefficient Examples ==
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{| class="wikitable"
{| class="wikitable"
|-
|-
! Shape !! \( c_d \)
! Shape !! <math>c_d</math>
|-
|-
| Smooth sphere (Re = \( 10^6 \)) || 0.1
| Smooth sphere (Re = <math>10^6</math>) || 0.1
|-
|-
| Rough sphere (Re = \( 10^6 \)) || 0.47
| Rough sphere (Re = <math>10^6</math>) || 0.47
|-
|-
| Flat plate perpendicular to flow (3D) || 1.28
| Flat plate perpendicular to flow (3D) || 1.28
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{| class="wikitable"
{| class="wikitable"
|-
|-
! Aircraft Type !! \( c_d \) !! Drag Count
! Aircraft Type !! <math>c_d</math> !! Drag Count
|-
|-
| F-4 Phantom II (subsonic) || 0.021 || 210
| F-4 Phantom II (subsonic) || 0.021 || 210
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== Drag Crisis ==
== 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 \( c_d \)).
At critical Reynolds numbers, <math>c_d</math> can drop dramatically due to a transition to turbulent boundary layer flow (e.g., golf ball dimples reduce <math>c_d</math>).


== See Also ==
== See Also ==
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Revision as of 11:06, 26 April 2025

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Drag Coefficient (commonly denoted as: , , or ) 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 is defined as:

where:

  • is the drag force.
  • is the mass density of the fluid.
  • is the flow velocity relative to the fluid.
  • 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), is typically lower.
  • For bluff bodies (e.g., brick, sphere), is higher due to flow separation and pressure drag.

Cauchy Momentum Equation

In terms of local shear stress and local dynamic pressure :

where:

  • = local shear stress.
  • , the dynamic pressure.

Drag Equation

The general drag force formula:

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: drops sharply at the critical Reynolds number.

Drag Coefficient Examples

General Shapes

Shape
Smooth sphere (Re = ) 0.1
Rough sphere (Re = Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle 10^6} ) 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 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, can drop dramatically due to a transition to turbulent boundary layer flow (e.g., golf ball dimples reduce ).

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

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