In classical mechanics, a reactive centrifugal force forms part of an action–reaction pair with a centripetal force.
In accordance with Newton's first law of motion, an object moves in a straight line in the absence of any external forces acting on the object. A curved path may however ensue when a force acts on it; this force is often called a centripetal force, as it is directed toward the center of curvature of the path. Then in accordance with Newton's third law of motion, there will also be an equal and opposite force exerted by the object on some other object,[1][2] such as a constraint that forces the path to be curved, and this reaction force, the subject of this article, is sometimes called a reactive centrifugal force, as it is directed in the opposite direction of the centripetal force.
Unlike the inertial force or fictitious force known as centrifugal force, which always exists in addition to the reactive force in the rotating frame of reference, the reactive force is a real Newtonian force that is observed in any reference frame. The two forces will only have the same magnitude in the special cases where circular motion arises and where the axis of rotation is the origin of the rotating frame of reference. It is the reactive force that is the subject of this article.[3][4][5][6]
Paired forces
A ball in circular motion held by a string tied to a fixed post.
The figure at right shows a ball in uniform circular motion held to its path by a string tied to an immovable post. In this system a centripetal force upon the ball provided by the string maintains the circular motion, and the reaction to it, which some refer to as the reactive centrifugal force, acts upon the string and the post.
Newton's first law requires that any body not moving in a straight line is subject to a force, and the free body diagram shows the force upon the ball (center panel) exerted by the string to maintain the ball in its circular motion.
Newton's third law of action and reaction states that if the string exerts an inward centripetal force on the ball, the ball will exert an equal but outward reaction upon the string, shown in the free body diagram of the string (lower panel) as the reactive centrifugal force.
The string transmits the reactive centrifugal force from the ball to the fixed post, pulling upon the post. Again according to Newton's third law, the post exerts a reaction upon the string, labeled the post reaction, pulling upon the string. The two forces upon the string are equal and opposite, exerting no net force upon the string (assuming that the string is massless), but placing the string under tension.
The reason the post appears to be "immovable" is because it is fixed to the earth. If the rotating ball was tethered to the mast of a boat, for example, the boat mast and ball would both experience rotation about a central point.
Applications
Even though the reactive centrifugal is rarely used in analyses in the physics literature, the concept is applied within some mechanical engineering concepts. An example of this kind of engineering concept is an analysis of the stresses within a rapidly rotating turbine blade.[1] The blade can be treated as a stack of layers going from the axis out to the edge of the blade. Each layer exerts an outward (centrifugal) force on the immediately adjacent, radially inward layer and an inward (centripetal) force on the immediately adjacent, radially outward layer. At the same time the inner layer exerts an elastic centripetal force on the middle layer, while and the outer layer exerts an elastic centrifugal force, which results in an internal stress. It is the stresses in the blade and their causes that mainly interest mechanical engineers in this situation.
A two-shoe centrifugal clutch. The motor spins the input shaft that makes the shoes go around, and the outer drum (removed) turns the output power shaft.
Another example of a rotating device in which a reactive centrifugal force can be identified used to describe the system behavior is the centrifugal clutch. A centrifugal clutch is used in small engine-powered devices such as chain saws, go-karts and model helicopters. It allows the engine to start and idle without driving the device, but automatically and smoothly engages the drive as the engine speed rises. A spring is used to constrain the spinning clutch shoes. At low speeds, the spring provides the centripetal force to the shoes, which move to larger radius as the speed increases and the spring stretches under tension. At higher speeds, when the shoes can't move any further out to increase the spring tension, due to the outer drum, the drum provides some of the centripetal force that keeps the shoes moving in a circular path. The force of tension applied to the spring, and the outward force applied to the drum by the spinning shoes are the corresponding reactive centrifugal forces. The mutual force between the drum and the shoes provides the friction needed to engage the output drive shaft that is connected to the drum.[7] Thus the centrifugal clutch illustrates both the fictitious centrifugal force and the reactive centrifugal force.
Difference from centrifugal pseudoforce
The "reactive centrifugal force" discussed in this article is not the same thing as the centrifugal pseudoforce, which is usually what's meant by the term "centrifugal force".
Reactive centrifugal force, being one-half of the reaction pair together with centripetal force, is a concept which applies in any reference frame. This distinguishes it from the inertial or fictitious centrifugal force, which appears only in rotating frames.
| Reactive centrifugal force | Inertial centrifugal force | |
|---|---|---|
| Reference frame |
Any | Only rotating frames |
| Exerted by |
Bodies undergoing rotation | Acts as if emanating from the rotation axis, it is a so-called fictitious force |
| Exerted upon |
The constraint that causes the inward centripetal force | All bodies, moving or not; if moving, coriolis force is present as well |
| Direction | Opposite to the centripetal force |
Away from rotation axis, regardless of path of body |
| Kinetic analysis | Part of an action-reaction pair with a centripetal force as per Newton's third law |
Included as a fictitious force in Newton's second law and is never part of an action-reaction pair with a centripetal force |
Gravitational two-body case
In a two-body rotation, such as a planet and moon rotating about their common center of mass or barycentre, the forces on both bodies are centripetal. In that case, the reaction to the centripetal force of the planet on the moon is the centripetal force of the moon on the planet.[6]
References
Roche, John (2001). "Introducing motion in a circle". Physics Education. 36: 399–405. Bibcode:2001PhyEd..36..399R. doi:10.1088/0031-9120/36/5/305.
Kobayashi, Yukio (2008). "Remarks on viewing situation in a rotating frame". European Journal of Physics. 29: 599–606. Bibcode:2008EJPh...29..599K. doi:10.1088/0143-0807/29/3/019.
Delo E. Mook & Thomas Vargish (1987). Inside relativity. Princeton NJ: Princeton University Press. p. 47. ISBN 0-691-02520-7.
J. S. Brar and R. K. Bansal (2004). A Text Book of Theory of Machines (3rd ed.). Firewall Media. p. 39. ISBN 9788170084181.
De Volson Wood (1884). The elements of analytical mechanics: solids and fluids (4th ed.). J. Wiley & sons. p. 310.
G. David Scott (1957). "Centrifugal Forces and Newton's Laws of Motion". 25. American Journal of Physics. p. 325.
Anthony G. Atkins, Tony Atkins and Marcel Escudier (2013). A Dictionary of Mechanical Engineering. Oxford University Press. p. 53. ISBN 9780199587438. Retrieved 5 June 2014.
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