Couple (mechanics)

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## Simple couple

## Independence of reference point

## Forces and couples

## Applications

## See also

## References

This article uses material from the Wikipedia page available here. It is released under the Creative Commons Attribution-Share-Alike License 3.0.

Couple Mechanics

In mechanics, a **couple** refers to two parallel forces that are equal in magnitude, opposite in sense and do not share a line of action.

A better term is **force couple** or **pure moment**. Its effect is to create rotation without translation, or more generally without any acceleration of the centre of mass. In rigid body mechanics, force couples are *free vectors*, meaning their effects on a body are independent of **torque**. This is not to be confused with the term torque as it is used in physics, where it is merely a synonym of moment.^{[1]} Instead, torque is a *special case* of moment. Torque has special properties that moment does not have, in particular the property of being independent of reference point, as described below.

- Definition

A couple is a pair of forces, equal in magnitude, oppositely directed, and displaced by perpendicular distance or moment.

The simplest kind of couple consists of two equal and opposite forces whose lines of action do not coincide. This is called a "simple couple".^{[2]} The forces have a turning effect or moment called a torque about an axis which is normal (perpendicular) to the plane of the forces. The SI unit for the torque of the couple is newton metre.

If the two forces are **F** and **-F**, then the magnitude of the torque is given by the following formula:

where

- is the moment of couple
*F*is the magnitude of the force*d*is the perpendicular distance (moment) between the two parallel forces

The magnitude of the torque is equal to *F d*, with the direction of the torque given by the unit vector , which is perpendicular to the plane containing the two forces and positive being a counter-clockwise couple. When **d** is taken as a vector between the points of action of the forces, then the torque is the cross product of **d** and **F**, i.e.

The moment of a force is only defined with respect to a certain point *P* (it is said to be the "moment about *P*"), and in general when *P* is changed, the moment changes. However, the moment (torque) of a *couple* is *independent* of the reference point *P*: Any point will give the same moment.^{[2]} In other words, a torque vector, unlike any other moment vector, is a "free vector".

(This fact is called *Varignon's Second Moment Theorem*.)^{[3]}

The proof of this claim is as follows: Suppose there are a set of force vectors **F**_{1}, **F**_{2}, etc. that form a couple, with position vectors (about some origin *P*) **r**_{1}, **r**_{2}, etc., respectively. The moment about *P* is

Now we pick a new reference point *P'* that differs from *P* by the vector **r**. The new moment is

Now the distributive property of the cross product implies

However, the definition of a force couple means that

Therefore,

This proves that the moment is independent of reference point, which is proof that a couple is a free vector.

A force *F* applied to a rigid body at a distance *d* from the center of mass has the same effect as the same force applied directly to the center of mass and a couple *Cl = Fd*. The couple produces an angular acceleration of the rigid body at right angles to the plane of the couple.^{[4]} The force at the center of mass accelerates the body in the direction of the force without change in orientation. The general theorems are:^{[4]}

- A single force acting at any point
*O?*of a rigid body can be replaced by an equal and parallel force*F*acting at any given point*O*and a couple with forces parallel to*F*whose moment is*M = Fd*,*d*being the separation of*O*and*O?*. Conversely, a couple and a force in the plane of the couple can be replaced by a single force, appropriately located.

- Any couple can be replaced by another in the same plane of the same direction and moment, having any desired force or any desired arm.
^{[4]}

Couples are very important in mechanical engineering and the physical sciences. A few examples are:

- The forces exerted by one's hand on a screw-driver
- The forces exerted by the tip of a screwdriver on the head of a screw
- Drag forces acting on a spinning propeller
- Forces on an electric dipole in a uniform electric field.
- The reaction control system on a spacecraft.
- Force exerted by hands on steering wheel.

In a liquid crystal it is the rotation of an optic axis called the *director* that produces the functionality of these compounds. As Jerald Ericksen explained

- At first glance, it may seem that it is optics or electronics which is involved, rather than mechanics. Actually, the changes in optical behavior, etc. are associated with changes in orientation. In turn, these are produced by couples. Very roughly, it is similar to bending a wire, by applying couples.
^{[5]}

**^***Physics for Engineering*by Hendricks, Subramony, and Van Blerk, page 148, Web link- ^
^{a}^{b}*Dynamics, Theory and Applications*by T.R. Kane and D.A. Levinson, 1985, pp. 90-99: Free download **^***Engineering Mechanics: Equilibrium*, by C. Hartsuijker, J. W. Welleman, page 64 Web link- ^
^{a}^{b}^{c}Augustus Jay Du Bois (1902).*The mechanics of engineering, Volume 1*. Wiley. p. 186. **^**J.L. Ericksen (1979) Timoshenko Acceptance Speech at iMechanica.org site for mechanicians

- H.F. Girvin (1938)
*Applied Mechanics*, §28 Couples, pp 33,4, Scranton Pennsylvania: International Textbook Company.

This article uses material from the Wikipedia page available here. It is released under the Creative Commons Attribution-Share-Alike License 3.0.

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