Air FrictionAir friction, or air drag, is an example of fluid friction. Unlike the standard model of surface friction, such friction forces are velocity dependent. The velocity dependence may be very complicated, and only special cases can be treated analytically. At very low speeds for small particles, air resistance is approximately proportional to velocity and can be expressed in the formwhere the negative sign implies that it is always directly opposite the velocity. For higher velocites and larger objects the frictional drag is approximately proportional to the square of the velocity: where is the air density, A the crosssectional area, and C is a numerical drag coefficient. |
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Linear Velocity DependenceFor objects moving at relatively low speeds through a liquid, where turbulence is not a significant factor, then the viscous resistance to the object's motion is approximately proportional to its velocity. Even in gases there are circumstances where the frictional resistance is approximately proportional to the velocity - such as the motion of tiny dist particles through the air. More commonly, air friction has terms proportional to the square or even higher powers of the velocity. For linear velocity dependence the resistance force can be written . If this resistance is the only force acting, then Newton's second law becomes
This terminal velocity is expressed in terms of an effective value of g if the buoyant force is significant. |
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Viscous ResistanceIf an object moves slowly through a liquid, it will experience a viscous drag which is approximately proportional to the velocity. For a sphere falling through a liquid in a velocity regime where viscosity is the dominant effect and turbulence can be neglected, the viscous drag is |
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Fluid FrictionThe resistance to an object's motion through a fluid may be termed "fluid friction." It may take the form of viscous resistance in a liquid, or the rather different character of air friction when an object moves through a gas. |
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