In this explainer, we will learn how to find the resultant of a system of parallel coplanar forces and how to locate its point of action.

Multiple forces that act at a point sum to a resultant force that acts at that point. The line of action of the resultant force intersects the lines of action of its components at the point where the forces act.

Consider, however, the forces shown in the following figure.

The forces shown do not act at the same point, and so, it is not immediately obvious what would be meant by the resultant of these forces. If a resultant can be defined for these forces, it is obvious that it will act in the same direction as either of the forces. What is not obvious is the position of the point that the resultant force will act at.

Let us suppose that the dashed line shown in the figure, which is perpendicular to the tails of the arrows representing the forces, is actually a light, thin rod. The forces would act on the rod to generate a net moment on the rod about points on the rod. The moment, , due to a force, , about a point equals the product of the magnitude of the force and the perpendicular distance, , from the line of action of the force to the point about which moments are taken. This can be expressed as

Let us assume that the forces shown in the figure have equal magnitudes. If moments are taken about the midpoint of the rod, , the forces produce moments about of equal magnitudes. One of the moments will be counterclockwise, hence positive, while the other will be clockwise, hence negative. The sum of these moments will be given by

The rod will, therefore, be in rotational equilibrium.

Let us now consider a force, , acting vertically downward on the rod with magnitude . Taking vertically upward as positive, the net force on the rod would be given by

acts to exactly oppose the upward forces and so satisfies a necessary condition for being the negative equivalent of the resultant of the upward forces. This is, however, not the only condition that must be satisfied. The action of the upward forces on the rod produces zero moment about , and so, for to be considered the negative equivalent of the resultant of the upward forces, it must also produce a zero net moment about .

must act at a particular point on the rod. Depending on the point at which acts, it may produce a nonzero moment about , and if produces a nonzero moment about , then cannot be considered to be the negative equivalent of the resultant of the upward forces. We can then ask: at what point, or points, on the rod can act that produces a zero net moment about ?

If acts at , the moment about due to is necessarily zero. If acts at any point other than , it produces a nonzero moment about . We see, therefore, that is the only point at which a force can act that allows it to be considered the negative equivalent to the resultant of the upward forces. This tells us that satisfies all necessary conditions to be considered to be the point at which the resultant of the upward forces acts. The line of action of the resultant of the upward forces is parallel to the upward forces and intersects , as shown in the following figure.

If the upward forces on the rod were not equal, the line of action of the resultant upward force would not be at , but there would still be a unique point corresponding to the point at which the resultant upward force acted. This would correspond to the point at which the clockwise and counterclockwise moments due to the upward forces were equal.

Let us look at an example where the resultant of unequal parallel forces is determined.

### Example 1: Finding the Resultant Force and Point of Action of Two Parallel Forces Acting in the Same Direction

Two parallel forces have magnitudes of 10 N and 20 N. The distance between their lines of action is 30 cm. If the two forces are acting in the same direction, find their resultant and the distance between its line of action and point .

### Answer

The magnitude of the resultant force is the sum of the magnitudes of the upward forces; hence,

The point at which acts is a point that is an element of . At , the moments due to the forces at and about are of equal magnitudes. The distance between and is 30 cm, and the distance between and is cm. At , it is the case that the moments due to the forces at and are given by

hence, and, therefore, where and are the magnitudes of the forces and and are the distances of the forces from the point of action of the resultant of the forces. The length of is 30 cm, so we have that

Let us now consider an example in which parallel forces act in opposite directions.

### Example 2: Finding the Resultant Force and Point of Action of Two Parallel Forces Acting in Opposite Directions

Two parallel forces have magnitudes of 24 N and 60 N as shown in the figure. The distance between their lines of action is 90 cm. Given that the two forces are acting in opposite directions, determine their resultant and the distance between its line of action and point .

### Answer

The magnitude of the resultant force is the sum of the magnitudes of the forces, where upward is taken as positive; hence,

At any point along , the moment due to either of the forces is either zero or clockwise. This tells us that there is no point along that can intersect the line of action of the resultant of the forces. This does not mean that the resultant of these forces cannot be defined, just that the line of action of the resultant is at a point that is not part of .

The point at which acts is a point . At , the moments due to the forces at and about are equal. The distance between and is 90 cm, and the distance between and is ; hence, at , where and are the magnitudes of the forces (with upward force taken as positive) and and are the distances of the forces from the point of action of the resultant of the forces. The length of is 90 cm, so we have that

We see from this that the line of action of the resultant of two parallel forces is not necessarily located between the lines of action of the forces. This can be understood as meaning that, for a light, thin rod of length 150 cm, if the forces in the question acted on the rod and an upward force of 36 N acted at the opposite end of the rod from , the rod would be in equilibrium. This is shown in the following figure.

Let us now look at an example in which the resultant of two parallel forces of unknown magnitudes is known.

### Example 3: Finding the Magnitude of Two Parallel Forces given Their Resultant and Point of Action

In the figure below, and are two parallel forces measured in newtons, where their resultant. If , , and , determine the magnitude of and .

### Answer

The moment about due to is zero, as acts at , and so the sum of the moments of and about must be zero.

The lines of action of and are not perpendicular to , so the moments due to and are the moments due to their components perpendicular to . The angle that the lines of action of and make with can be denoted by as shown in the following figure.

We note that the resultant force, , is given by

The moments due to the resultant force and due to act clockwise, while the moment due to acts counterclockwise; hence, the moment about due to is given by

The length of is given by and so, the moment about due to is given by

The moments about sum to zero, where is positive and is negative, so we can see that

The factor of can be eliminated by dividing both sides of the equation by , leaving

The magnitude of the resultant force is the sum of the magnitudes of the forces, where upward is taken as positive; hence,

This expression can be rearranged to give an expression for in terms of :

Let us now look at an example in which the resultant of an arbitrary number of parallel forces is determined.

### Example 4: Finding the Resultant and Point of Action of Five Parallel Forces

Points , , , , and are lying in the same straight line such that , , , and . Five forces of magnitudes 40, 25, 20, 45, and 50 newtons are acting as shown in the figure. Determine their resultant and the distance between its line of action and point .

### Answer

The magnitude of is given by the sum of the forces acting. Taking upward as positive, this is given by

We can define a parameter that is equal to the distance in the positive -direction between the line of action of the 40-newton force and the line of action of . The moment due to the 40-newton force is therefore given by

The distance between the lines of action of the other forces and the line of action of can also be expressed in terms of . For example, the line of action of the 25-newton force has a distance from of 8 cm in the positive -direction. The distance between the line of action of and the line of action of the 25-newton force is given by

The moment due to the 25-newton force is, therefore, given by

Expressing the moments due to all of the forces this way, we obtain

The sum of the moments due to the forces is zero. If we distribute the parentheses throughout, then separate the integer terms from the terms that are multiples of , we find that

Let us now look at an example in which two parallel forces are represented by their perpendicular components.

### Example 5: Finding the Resultant and Point of Action of Two Parallel Forces Given in Vector Form

Given that the two parallel forces and are acting at and , respectively, determine their resultant , and find its point of action.

### Answer

The magnitudes of the componentsβ resultant force is the sum of the magnitudes of the components of the forces, where upward is taken as positive; hence,

The following figure shows the forces acting at and .

There is an angle of magnitude between the line of action of either force and a line that intersects the points of action of both forces. It is possible to determine from the information in the question, but this is actually not necessary. Determining the point at which the resultant acts will require determining the ratios of the moments due to the forces about this point. Multiplying both forcesβ magnitudes by will not change this ratio.

The magnitude of is given by

The magnitude of is given by

The forces do not act perpendicularly to , so the components of the forces perpendicular to are given by and

The force components acting perpendicularly to can be shown with drawn horizontally, as shown in the following figure, which also shows the distance of from .

We can see from the figure that the lines from and that are parallel to the - and -axes, respectively, both have a length of 8. These lines are perpendicular and so form two legs of a right triangle that has a hypotenuse with a length given by

From the figure, we can see that , the distance along from , to the point at which the resultant acts, is given by equating the moments due to the forces at and at :

The factor of can be eliminated by dividing both sides of the equation by , leaving

This expression for can be simplified as follows:

The length of is , so the resultant acts at a point that is at a distance from in the direction of .

The distance of from is 8 in the -direction and is also 8 in the -direction; hence, the point of action of is at a distance of in both the - and -directions from . The coordinates of the point of action of are therefore given by

Let us summarize what we have learned in these examples.

### Key Points

- The point of action of the resultant of multiple parallel forces is the point at which the moments about the point due to the forces sum to zero.
- If the perpendicular distance between the lines of action of parallel forces is a line segment , the point of action of the resultant of the forces is not necessarily an element of .
- The position of the point of action of the resultant of parallel forces is not affected by the angle between the lines of action of the forces and the line that intersects the points of action of the forces.