Drag Force

Types of Drag Force

There are different types of drag force, especially when considering the flight of airplanes:

• Parasitic Drag—Drag caused by the object's shape, material, and construction type.
  • Form Drag—The drag due to the shape of the object moving through the fluid.
  • Skin Friction Drag—The drag due to the roughness of the object's surface.
  • Interference Drag—The drag resulting from two airflows of different speeds meeting and interfering.
• Induced Drag—The drag resulting from lift.
• Wave Drag—The drag due to shockwaves.

Phew, that was a lot of information to trudge through, if word density could be considered, this article would have a massive drag force.

Examples of Drag Force

Here we go again—even more examples. It's like walking through honey.

Drag is present when there is relative motion between an object and a fluid. Some examples of drag force include the following:

• Any object falling through the air. For example, skydivers use principles of drag force to move and position themselves through the air, and when they open their parachutes, the greater drag force that's created helps slow them down to land.
• Drag force slows down cars, planes, and ships when they move. So engineers increase the aerodynamics of these vehicles to reduce drag and increase the vehicles' efficiency.
• Swimmers fight against drag force when they swim. Even shaving can reduce drag and increase swimmers' speeds.
• Flying squirrels use their wing-like skin to use drag force to control their flight and landings.
• If you were to stand on top of a quickly moving train, it wouldn't be as easy to stand or run as many movies make it seem because there would be a drag force pushing against you.
• Drag force causes kites to fly. You must run forward with the kite to get the drag force to push against it and lift it into the air.

Drag Force Equation

The common equation or formula for drag force is shown below:

$$D=\frac{1}{2}\\C\rho Av^2\mathrm{.}$$

This equation is only accurate under certain conditions: the motion is fast enough that the fluid behind the object is turbulent, the fluid is not denser than air, and the object is not tiny. As with other forces, drag force is measured in \(\mathrm{newtons}\) \(\mathrm{N}\).

Drag Force Formula

Above, you probably saw a bunch of variables that you have never seen before. To aid you in understanding what the drag force is, we'll go over each of these variables.

\(C\) is the coefficient of drag, which is a unitless number that has been determined experimentally. \(\rho\) represents the density of the fluid in \(\mathrm{kg/m^3}\); as the density increases, the drag force increases. In our opening example, water contributes to a higher drag force than air because it has a higher density.

\(A\) is the effective cross-sectional area of the object in \(\mathrm{m^2}\)—this is the area of the object that is perpendicular to the motion. So, for example, when sticking your hand outside a moving car's window, if you tilt your hand, so the side is facing the front of the car, you will feel less force than if you stick your hand out with the palm facing the front: this is because your hand has a smaller cross-section in the first orientation.

\(v\) is the relative velocity between the object and the fluid in \(\mathrm{m/s}\). If you put your hand in water and slam it down, you will feel more of a force fighting against you than if you slowly lower it. Drag force differs from friction because friction doesn't depend on the object's speed.

Stokes's Law

Have you enjoyed the terrible puns so far? I don't mean to stoak the fire burning in your heart even more from all these dad jokes, but I just have to.

When the conditions don't meet the requirements listed above, we can use Stokes's Law to find the friction force:

$$F_s = 6\pi \eta r v$$

where \(\eta \) is the viscosity of the fluid in SI units of Pascal-seconds \(\mathrm{Pa\,s}\), which is the same as kilograms per meter-second \(\mathrm{kg/m\,s}\), \(r\) is the radius of the object in meters, and \(v\) is the velocity in meters per second \(\mathrm{m/s}\). In this case, the drag force is proportional to the velocity rather than the velocity squared. With this equation, the drag force may be referred to as a viscous drag force, where the drag force is dependent on the fluid's viscosity.

Drag Force in Free-Fall—Terminal Velocity

If you drop a bouncy ball off the empire state building, initially the force acting against the ball is negligible since the velocity starts at zero. Instead, the main force acting on it is the force of gravity, which pulls it down and causes it to accelerate. As the velocity increases, the drag force acting against the ball's fall will increase. This opposite force causes the ball's acceleration to slow until, eventually, the drag force equals the force of gravity and the ball no longer accelerates. At this point, the ball will reach a constant speed at its terminal velocity.

Example Problem Using Drag Force

Now, it's time for an example.

Hopefully, finishing this article wasn't too much of a drag—more like walking through a luscious breeze rather than cold honey. If your answer was the honey, don't panic, you're almost done: here are the most important points you need to remember.