Math 2.0

Mechanics of particles and systems Definition

Couple

Builds on TorqueCross product

Definition

Let F∈ℝ3F \in \R^3 be nonzero, and let p1,p2∈ℝ3p_1, p_2 \in \R^3 be points such that p1−p2p_1 - p_2 is not parallel to FF. The pair of forces FF acting at p1p_1 and −F-F acting at p2p_2 is a couple. Its moment is the vector M=(p1−p2)×F,M = (p_1 - p_2) \times F, where ×\times is the cross product.

Remarks

For every reference point OO, the total torque of the pair is (p1−O)×F+(p2−O)×(−F)=M(p_1 - O) \times F + (p_2 - O) \times (-F) = M, so the moment does not depend on OO. Its size is ∣F∣d\abs{F} d, where dd is the distance between the two lines of action.

Example: F=(0,5,0)F = (0, 5, 0) at p1=(0.2,0,0)p_1 = (0.2, 0, 0) and −F-F at p2=(−0.2,0,0)p_2 = (-0.2, 0, 0) form a couple with moment (0.4,0,0)×(0,5,0)=(0,0,2)(0.4, 0, 0) \times (0, 5, 0) = (0, 0, 2).

Non-example: if p1−p2p_1 - p_2 is parallel to FF, the two forces act along the same line, and their moment is 00; they cancel completely and do not form a couple. Two couples with the same moment have the same effect on a rigid body, so a couple is often identified with its moment, a free vector.

Reading path

To understand this page from the ground up, read these 4 pages in order. The foundations come first.

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Each page uses the pages above it. The colour of the bar on a box shows how strong the evidence is, and the box also gives it as text. The list has the same pages.
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  1. Euclidean vector concept
  2. Torque concept
  3. Cross product definition
  4. Couple definition

Further reading

  1. Web https://en.wikipedia.org/wiki/Couple_(mechanics)
About this page
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URIm2://3VP4W3XFQS
Kinddefinition
WritingW0 stub
MSC70C20
DefinesCouple
UsesTorque, Cross product
Changed3 November 2026

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