The Physics Of Roller Coasters

Amusement parks are a place where people of all ages go to enjoy themselves and relax, but if there’s one thing that captures the attention of both children and adults alike, it’s roller coasters! Personally, this makes me wonder what it is about roller coasters that provides such widespread excitement to so many of us, but such dreadful fear in others. The reason for these intense emotions is not due to the speed that one experiences, but rather the forces and the feeling of weightlessness that affect riders. Let’s now take a look at the physics of roller coaster loops to reach an understanding of how one experiences the powerful forces and the notion of weightlessness.

roller-coaster

(Photo credit: Pixabay)

Physics of Loops

circle

The primary force that makes one feel a particular set of sensations is the acceleration, and the section of a roller coaster that exploits this acceleration (more accurately known as centripetal acceleration) are the clothoid loops. A clothoid loop assumes the geometric shape of a teardrop. A clothoid is a section of a spiral that has a continually changing radius. Unlike a circular loop, which has a constant radius, a clothoid loop has a greater radius at the bottom of the loop than at the top. To make the envisioning of the clothoid loop easier, let’s imagine two circles of the same radius that overlap one another to form the base of the clothoid, while a smaller circle forms the radius at the top of the clothoid.

roller coaster gif

As the roller coaster cart passes through the clothoid loop, one experiences acceleration based on two main factors: the constant change in direction and the constant change in speed. A rightward moving roller coaster car gradually becomes an upward moving roller coaster car and a leftward moving roller coaster car, then a downward moving roller coaster car. In other words, there is a continuous change in the direction of the roller coaster car as it moves through the clothoid loop. As the roller coaster car begins to ascend the loop, it begins to slow down. An increase in height leads to an increase in potential energy, which results in a decrease in kinetic energy and speed. Conversely, a reduction in height increases kinetic energy and speed, so the roller coaster car experiences the highest speeds at the bottom of the loop—both upon entering and leaving the loop—and the lowest speeds at the top of the loop.

Force Analysis of a Loop

Whenever an object moves in a closed curved path, it experiences a net inward acceleration that results in the object experiencing a net inward force. Before we proceed any further with the analysis of what forces a person experiences on a roller coaster, we will assume that the roller coaster car does not experience any friction or air resistance. With that in mind, there will be two forces that act upon the roller coaster car:  the FORCE OF GRAVITY (FGRAV) and the Normal Force (FNORMAL). The normal force is directed in the direction of the track, while the gravitational force is always directed downwards. At the bottom of the loop, the track pushes upwards on the car with a normal force. However, at the top of the loop, the normal force is directed downwards; since the track (the supplier of the normal force) is above the car, it pushes downwards on the car. The free-body diagrams for these two positions are shown in the diagrams at the right.

The magnitude of the force acting on the roller coaster car (or passenger) can be calculated using the formula FGRAV=m.g, where the acceleration due to gravity is represented by g (where g=9.8 m/s2). The magnitude of the normal force depends on three factors—the speed of the car, the radius of the loop, and the mass of the rider. As depicted in the free body diagram, the magnitude of FNORMAL is always greater at the bottom of the loop than it is at the top. The normal force must always be of the appropriate size to combine with the FGRAV in such a way to produce the required inward or centripetal net force. At the bottom of the loop, the Fgrav points outwards, away from the center of the loop. The normal force must be sufficiently large to overcome this FGRAV and supply some excess force to result in a net inward force. In a sense, FGRAV and FNORMAL are in a tug-of-war and FNORMAL must win by an amount that is equal to the net force. At the top of the loop, both FGRAV and FNORMAL are directed inwards. FGRAV is found in the usual way (using the equation FGRAV =m*g). Once more, the FNORMAL must provide sufficient force to produce the required inward or centripetal net force.

Sensations Of Weightlessness

When you are on a roller coaster ride and travel through a loop, you will likely experience a small normal force at the top of the loop and a sizable normal force at the bottom of the loop. The normal force provides the feeling of a person’s weight. The more you weigh, the more normal force you will experience when at rest in your seat. However, when you board a roller coaster ride and accelerate through the clothoid loops, you will feel a normal force that is continually changing and one to which you are not accustomed.

This normal force provides a sensation of weightlessness or weightiness. At the top of the loop, a person will feel partially weightless if the normal forces become less than the person’s weight. At the bottom of the loop, a rider will instead feel very heavy due to the increased normal forces. It’s important to realize that the force of gravity and the weight of your body are not changing; only the magnitude of the normal supporting force is constantly changing.

With all of that information in mind, next time you go on a roller coaster, you’ll know why you feel a certain way, whether that is ecstatic, scared…. or just nauseous!

References:

  1. Physics of Roller Coasters
  2. HowStuffWorks
  3. Explain That Stuff
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About the Author:

Venkatesh is an Electrical and Electronics Engineer from SRM Institute of Science and Technology, India. He is deeply fascinated by Robotics and Artificial Intelligence. He is also a chess aficionado, He likes studying chess classics from the 1800 and 1900’s. He enjoys writing about science and technology as he finds the intricacies which come with each topic fascinating.

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