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Boundless Physics
The Laws of Motion
Further Applications of Newton's Laws
Physics Textbooks Boundless Physics The Laws of Motion Further Applications of Newton's Laws
Physics Textbooks Boundless Physics The Laws of Motion
Physics Textbooks Boundless Physics
Physics Textbooks
Physics
Concept Version 8
Created by Boundless

Drag

The drag force is the resistive force felt by objects moving through fluids and is proportional to the square of the object's speed.

Learning Objective

  • Relate the magnitude of drag force to the speed of an object


Key Points

    • Objects moving through a fluid feel a force which resists their motion. This force is known as the drag force.
    • The drag force is proportional to the square of the velocity of the object relative to the fluid.
    • The equation for drag is $F_D = \frac{1}{2} C \rho A v^2$. $C$ is a constant called the drag coefficient. $\rho$ is the density of the fluid. $A$ is the surface area in the direction of motion.

Term

  • fluid

    Any substance which can flow with relative ease, tends to assume the shape of its container, and obeys Bernoulli's principle; a liquid, gas or plasma.


Full Text

Another interesting force in everyday life is the force of drag on an object when it is moving in a fluid (either a gas or a liquid). You feel the drag force when you move your hand through water. You might also feel it if you move your hand during a strong wind. The faster you move your hand, the harder it is to move. You feel a smaller drag force when you tilt your hand so only the side goes through the air—you have decreased the area of your hand that faces the direction of motion. 

Like friction, the drag force always opposes the motion of an object. Unlike simple friction, the drag force is proportional to some function of the velocity of the object in that fluid. This functionality is complicated and depends upon the shape of the object, its size, its velocity, and the fluid it is in. Aerodynamic objects tend to have small surface areas and be designed to have low drag coefficients.

For most large objects such as bicyclists, cars, and baseballs not moving too slowly, the magnitude of the drag force $F_D$ is found to be proportional to the square of the speed of the object. We can write this relationship mathematically as $F_D \propto v^2$. When taking into account other factors, this relationship becomes $F_D = \frac{1}{\frac{2C}{rho A v^2}}$, where $C$ is known as the drag coefficient, a unit-less number that represents the aerodynamic properties of the object, $A$ is the cross-sectional area of the object which is facing the direction of motion, and $\rho$ is the density of the fluid the object is moving through.

Aerodynamic Shape

From racing cars to bobsled racers, aerodynamic shaping is crucial to achieving top speeds. Bobsleds are designed for speed. They are shaped like a bullet with tapered fins. (credit: U.S. Army, via Wikimedia Commons)

Retarding and Drag Forces

A brief look at retarding (drag) forces in physics, for students in introductory physics classes that use calculus. This video walks through a single scenario of an object experiencing a drag force where the drag force is proportional to the object's velocity.

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