# Parallelogram of force

The **parallelogram of forces** is a method for solving (or visualizing) the results of applying two forces to an object.

When more than two forces are involved, the geometry is no longer parallelogrammatic, but the same principles apply. Forces, being vectors are observed to obey the laws of vector addition, and so the overall (resultant) force due to the application of a number of forces can be found geometrically by drawing vector arrows for each force. For example, see Figure 1. This construction has the same result as moving **F**_{2} so its tail coincides with the head of **F**_{1}, and taking the net force as the vector joining the tail of **F**_{1} to the head of **F**_{2}. This procedure can be repeated to add **F**_{3} to the resultant **F**_{1} + **F**_{2}, and so forth.

## Newton's proofEdit

### Preliminary: the parallelogram of velocityEdit

Suppose a particle moves at a uniform rate along a line from A to B (Figure 2) in a given time (say, one second), while in the same time, the line AB moves uniformly from its position at AB to a position at DC, remaining parallel to its original orientation throughout. Accounting for both motions, the particle traces the line AC. Because a displacement in a given time is a measure of velocity, the length of AB is a measure of the particle's velocity along AB, the length of AD is a measure of the line's velocity along AD, and the length of AC is a measure of the particle's velocity along AC. The particle's motion is the same as if it had moved with a single velocity along AC.^{[1]}

### Newton's proof of the parallelogram of forceEdit

Suppose two forces act on a particle at the origin (the "tails" of the vectors) of Figure 1. Let the lengths of the vectors **F**_{1} and **F**_{2} represent the velocities the two forces could produce in the particle by acting for a given time, and let the direction of each represent the direction in which they act. Each force acts independently and will produce its particular velocity whether the other force acts or not. At the end of the given time, the particle has *both* velocities. By the above proof, they are equivalent to a single velocity, **F**_{net}. By Newton's second law, this vector is also a measure of the force which would produce that velocity, thus the two forces are equivalent to a single force.^{[2]}

## Bernoulli's proof for perpendicular vectorsEdit

We model forces as Euclidean vectors or members of . Our first assumption is that the resultant of two forces is in fact another force, so that for any two forces there is another force . Our final assumption is that the resultant of two forces doesn't change when rotated. If is any rotation (any orthogonal map for the usual vector space structure of with ), then for all forces

Consider two perpendicular forces of length and of length , with being the length of . Let and , where is the rotation between and , so . Under the invariance of the rotation, we get

Similarly, consider two more forces and . Let be the rotation from to : , which by inspection makes .

Applying these two equations

Since and both lie along , their lengths are equal

which implies that has length , which is the length of . Thus for the case where and are perpendicular, . However, when combining our two sets of auxiliary forces we used the associativity of . Using this additional assumption, we will form an additional proof below.^{[3]}^{[4]}

## Algebraic proof of the parallelogram of forceEdit

We model forces as Euclidean vectors or members of . Our first assumption is that the resultant of two forces is in fact another force, so that for any two forces there is another force . We assume commutativity, as these are forces being applied concurrently, so the order shouldn't matter .

Consider the map

If is associative, then this map will be linear. Since it also sends to and to , it must also be the identity map. Thus must be equivalent to the normal vector addition operator.^{[3]}^{[5]}

## ControversyEdit

The mathematical proof of the parallelogram of force is not generally accepted to be mathematically valid. Various proofs were developed (chiefly *Duchayla's* and *Poisson's*), and these also caused objections. That the parallelogram of force was true was not questioned, but *why* it was true. Today the parallelogram of force is accepted as an empirical fact, non-reducible to Newton's first principles.
^{[3]}^{[6]}

## See alsoEdit

## ReferencesEdit

**^**Routh, Edward John (1896).*A Treatise on Analytical Statics*. Cambridge University Press. p. 6., at Google books**^**Routh (1896), p. 14- ^
^{a}^{b}^{c}Spivak, Michael (2010).*Mechanics I*. Physics for Mathematicians. Publish or Perish, Inc. pp. 278–282. ISBN 0-914098-32-2. **^**Bernoulli, Daniel (1728).*Examen principiorum mechanicae et demonstrationes geometricae de compositione et resolutione virium*.**^**Mach, Ernest (1974).*The Science of Mechanics*. Open Court Publishing Co. pp. 55–57.**^**Lange, Marc (2009). "A Tale of Two Vectors" (PDF).*Dialectica, 63*. pp. 397–431.