---
title: "Force-couple system at A; couple is free vector"
subject: "Applied Mechanics"
chapter: 3
key: "semester_1/applied_mechanics:force-couple-system-point-a-box-couple-free-vector"
source: https://www.bctengineer.com/q/semester_1/applied_mechanics/force-couple-system-point-a-box-couple-free-vector
site: BCT Engineering
---

# Force-couple system at A; couple is free vector

Applied Mechanics · Chapter 3: Forces acting on particle and rigid body

- Asked in: 2071 Shrawan, 8+3 marks
- Video: [7.1 Replacing a Force with an equivalent Force-Couple system](https://www.youtube.com/watch?v=CFVwNRgCy3Q) — Vector In Motion
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_1/applied_mechanics/force-couple-system-point-a-box-couple-free-vector
- Whole chapter: https://www.bctengineer.com/md/semester_1/applied_mechanics/chapter-3

## Question

Find the resultant of force couple system at point A as shown in figure below. Take F1 = 100 kN, F2 = 300 kN. Define a couple and show that couple is a free vector. [Figure: box with origin O, axes x, y, z, dimensions 4 m, 5 m, 3 m, 2 m, 1 m, 1.5 m; forces 50 kN, 50 kN, 200 kN, 200 kN, 300 kN, 300 kN, 20 kN (two), F1 and F2 as shown, A at the lower corner on the z axis.]

## Short answer

The force-couple system at A is R = 280 kN (components -141.4i+226.3j-84.9k kN) with M_A = 918 kN·m (-320.3i+424.3j+748.5k kN·m). A couple is two equal opposite parallel forces producing pure rotation; its moment is a free vector because its value is independent of the reference point.

## Answer

**Reading of the figure:** the box is x = 5 m, y = 4 m, z = 3 m with O at the back corner and A = (0, 0, 3). The loads are:
- F₁ = 100 kN along the space diagonal from O to (5, 4, 3), and F₂ = 300 kN along the diagonal from (5, 0, 3) to (0, 4, 0).
- 20 kN up at (5, 4, 0) and 20 kN down at A (a couple).
- A pair of 50 kN vertical forces 2 m apart on the left top edge: couple with moment 100 kN·m, −x sense.
- A pair of 200 kN horizontal forces (along x) 1 m apart: couple 200 kN·m, −z sense.
- A pair of 300 kN forces (along z) 1.5 m apart on the right face: couple 450 kN·m, −x sense.

#### Forces
F₁ = 100 (5, 4, 3)/√50 = (70.71, 56.57, 42.43) kN
F₂ = 300 (−5, 4, −3)/√50 = (−212.13, 169.71, −127.28) kN
The two 20 kN forces cancel (zero resultant) but form a couple.

**Resultant force at A:**
R = F₁ + F₂ = (−141.42, 226.27, −84.85) kN, |R| = **280 kN**

#### Moment about A (r × F)
```text
F1 acts at O:       r = (0,0,−3)   -> ( 169.71, −212.13,   0.00)
F2 acts at (5,0,3): r = (5,0,0)    -> (   0.00,  636.40, 848.53)
20 kN pair:         r = (5,4,−3)   -> (  60.00,    0.00, 100.00)
50 kN pair                           -> (−100.00,   0.00,   0.00)
200 kN pair                          -> (   0.00,   0.00, −200.00)
300 kN pair                          -> (−450.00,   0.00,   0.00)
------------------------------------------------------------------
M_A                                  = (−320.3,  424.3,  748.5) kN·m
```
|M_A| = **918 kN·m**

**Answer: the force-couple system at A is R = (−141.4 i + 226.3 j − 84.9 k) kN together with M_A = (−320.3 i + 424.3 j + 748.5 k) kN·m.**

#### Couple
A couple is a pair of equal, opposite and parallel forces whose lines of action do not coincide. It produces pure rotation, no translation, because the resultant force is zero. Its moment is M = F × d, where d is the perpendicular distance between the forces (the arm of the couple). It is a vector perpendicular to the plane of the couple.

#### A couple is a free vector
Let forces **F** at A and **−F** at B form a couple. Take any point O, with position vectors r_A and r_B.
```text
Moment about O = r_A × F + r_B × (−F)
               = (r_A − r_B) × F
               = r_AB × F
```
The result contains only the vector r_AB between the two points of application. It does not contain the position of O. So the moment of a couple is the same about every point. The couple can be moved anywhere in its plane, to a parallel plane, or turned in its plane, without a change in its effect on a rigid body, provided magnitude and direction of the moment vector remain the same. Hence its moment is a **free vector**.

## Check yourself

The answer's key points as multiple-choice questions, with the correct option and why.

1. How is F1 = 100 kN along the diagonal from O to (5, 4, 3) written as a vector?
   A. 100 × (5, 4, 3)/sqrt(50)
   B. 100 × (5, 4, 3)
   C. 100 × (5, 4, 3)/12
   D. 100 × (1, 1, 1)
   Answer: A. Force vector = magnitude × direction vector divided by its length (sqrt(25+16+9)). (Key point: Unit vector for F1)

2. What is the effect of the two 20 kN forces (one up, one down)?
   A. They add nothing to R but form a couple
   B. They double R
   C. They cancel completely with no effect
   D. They add 40 kN to R
   Answer: A. Equal and opposite forces sum to zero but, being on different lines, give a couple. (Key point: Pair of 20 kN forces)

3. How are the couple pairs added to M_A?
   A. Their moment vectors are added directly, since a couple's moment is the same about any point
   B. Each is multiplied by its distance from A
   C. Only the largest couple is included
   D. They are added to R
   Answer: A. A couple is a free vector, so its moment doesn't depend on A. (Key point: Adding couples)

4. What step shows a couple's moment doesn't depend on the reference point O?
   A. r_A × F + r_B × (-F) = (r_A - r_B) × F, which has no O
   B. F is the same for both forces
   C. r_A and r_B are both zero
   D. The sum of forces is nonzero
   Answer: A. The result r_AB × F contains only the vector between the two points of application. (Key point: Free vector proof)

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