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# Equilibrium of Forces

## Introduction

Simply put, an equilibrium of forces is a situation when forces are placed at both ends of a body to stop it from moving or rotating (to balance its position). The force helps the body to remain in a balanced position.

In physics, we usually say that the forces have canceled each other so that the body can stay in EQUILIBRIUM.

For example, when two children sit on the two ends of a seesaw. If the weight of both children is the same, the seesaw would remain in equilibrium.

But if their weight is not the same, the child with a higher weight would go down while a child with a lower weight would move up.

Another example of bodies in equilibrium is the tug-of-war game. Two groups of people are expected to hold a rope from both ends. The rope is separated by a line at the center. For a group to win, they must pull the rope to make the other group cross into their line.

If both groups failed to pull each other, we can now say that they are at equilibrium and their forces have canceled each other.

Therefore, for a body to remain at equilibrium, the net forces acting on the body must cancel each other.

The above explanation takes us to the statement: “The sum of the forces moving the body in one direction is equal to the sum of the forces pushing the body in the opposite direction”.

Additionally, for an object to remain in equilibrium, the vector sum of all relevant forces acting upon the object must be zero. Thus, the object cannot accelerate in an inertial frame of reference.

## Forms of Equilibrium

We have three forms of equilibrium, and they are:

1. Dynamic or Kinetic Equilibrium
2. Static Equilibrium, and
3. Thermal Equilibrium

### Static Equilibrium

When forces acting on a body have the same magnitude and direction, they would help the body to remain at equilibrium.

Therefore, for a body to maintain static equilibrium, the sum of the forces acting on the body must be at rest. This implies that its net force is zero.

An Example of static equilibrium is a student bag sitting on the desk. The bag is pulled downward by gravitational force. At the same time, the desk exerts an equal and opposite force (upward force) to cancel the downward force of the bag.

The above example helps us to understand that the sum of the forces from both the bag and the desk is zero. Hence, they canceled each other so that the bag could remain on the desk.

In static equilibrium, the body is static and does not move. This is because all the forces acting on the body are the same.

### Dynamic or Kinetic Equilibrium

In the case of dynamic equilibrium, the body moves with a constant velocity, and a zero net force or torque acting upon it.

The body undergoes translational motion with a constant velocity or rotates with a constant angular velocity about a fixed point.

Therefore, both forces that initiate and resist the motion are balanced.

For Example, a relationship between a car engine and a tarred road. The car engine helps the car to move on the tarred road, while the road resists the movement of the car. Consequently, the force of friction on the tarred road would try to oppose the movement of the car forward.

The two forces from the engine of the car and the friction of the tarred road will continue to cancel each other. Hence, both forces are in dynamic equilibrium.

The state of dynamic equilibrium helps the body to maintain constant velocity on the road. Your car will slow down if the friction is greater than the force of the engine. However, if the force of the engine is greater than the friction on the road, the car will accelerate.

### Thermal Equilibrium

Temperature is the degree of hotness or coldness of a body. The coldness of a body signifies its low temperature, while the hotness of a body marks its high temperature. Therefore, when the temperature of a body rises from its lowest to a high degree, energy in the form of heat is transferred.

However, for a body to be in thermal equilibrium. The heat energy between the thermodynamic bodies must cancel each other. Hence, when the net flow of the heat energy is zero, the heat will stop flowing in the system.

## State of Equilibrium

Here are some conditions for a body to be at equilibrium:

1. The entire body remains at rest (motionless) or undergoes translational motion at constant velocity.
2. The body either stops rotating or rotates at a constant angular velocity.

## Resultant of Forces

When a body is under the influence of multiple forces, the resultant force is a force that when acting alone will have the same effect in magnitude and direction as the other forces acting together.

We use the symbol R to represent the resultant forces. Additionally, we apply the law of parallelogram to find the resultant forces.

When you have two forces A and B hanging at a point C. The resultant of the forces A and B at point C is calculated by applying the law of parallelogram.

The resultant of the two forces A and B have the same magnitude. However, the direction of forces A and B opposes the direction of the force at point C.

## Equilibrant of Forces

This is a force that cancels other forces. It has the same magnitude with resultant force, but they move in opposite directions.

To explain equilibrant, let’s assume we have three forces F1, F2, and F3 at equilibrium. The resultant of any two forces are equal but opposite in direction to one of the third forces.

Here is how it goes:

1. The equilibrant of F1 and F2 is F3
2. The equilibrant of F1 and F3 is F2
3. The equilibrant of F2 and F3 is F1

## Principles of Triangle of Forces

The principle of the triangle of forces states that if three forces are in equilibrium, they can be represented in both magnitude and direction by the three sides of a triangle taken in order.

## Moment of a Force

The moment is the turning effect of forces about an axis or point. The moment is the product of a force and the perpendicular distance of its line of action.

## Principle of moment

The principle of moment states that if a body is in equilibrium, then the sum of the clockwise moments about any point on the body is equal to the sum of the anticlockwise moments about the exact point.

## What is the Difference between Clockwise and Anticlockwise moments?

A clockwise moment is a rotational force that makes an object rotate in a clockwise direction. The anticlockwise moment is also a rotational force that makes an object rotate in the counterclockwise direction. The direction of rotation is determined by the direction of the force and the position of the object in relation to the force.

For example, we all know that a wall clock works by rotating in the right direction. Hence, when an object rotates in the direction of the clock, we say that it rotates in the clockwise direction.

The same scenario applies to anticlockwise moments. But in this case, the direction of the clock is assumed to rotate in the left direction. Thus, when an object’s rotation opposes the clockwise rotation. We can say that it moves counterclockwise or anticlockwise.

## Couples

This is a pair of equal and parallel forces acting on a body in opposite directions and whose line of action does not meet. It produces the rotation of an object about a point.

## Torque

The torque is the turning effect of a couple. It is the product of force and the perpendicular distance between the line of action of the two forces. Torque is a vector quantity and its unit is a newton-meter (Nm).

## Parallel of Forces

Here are a few conditions for the equilibrium of rigid objects:

### Under the action of Parallel forces

1. The sum of the forces in one direction is equal to the sum of the forces in the opposite direction. Total downward force is equal to the total upward force.
2. The sum of the clockwise moment of forces about any point is equal to the sum of the anticlockwise moment of the forces about the same point. The algebraic sum of the moment about any point is zero. It’s also important to know that the clockwise direction represents a negative sign while the anticlockwise moment represents a positive sign.
3. The resultant force must be zero.

### Under the Action of Non-Parallel Forces

1. The line of action of the forces must coincide
2. The resultant should be zero
3. The algebraic sum of resolved components of the forces in any perpendicular direction is respectively zero.

### Three Non-Parallel Coplanar Force

1. If any object is in equilibrium under the actions of three forces, the resultant of the two forces must be equal and opposite to the third force.
2. The lines of action of the forces must coincide at a point.
3. All three forces must coincide.
4. The third force’s line of action must go through the point where the lines of action of the other two forces intersect.
5. The sum of the forces at a point must add up to zero.
6. The forces can be represented in a magnitude and direction by the sides of a triangle taken in order.

## Centre of Gravity

This is a point through which the resultant weight of the body appears to concentrate. We can also define center of gravity as the point at which the weight of a body acts, regardless of the body’s position.

## Types of Equilibrium

There are three types of equilibrium:

1. Stable Equilibrium: A body regains its original position after slight displacement. A large bottom and a low center of gravity would make an object maintain a stable equilibrium. A television on a TV stand is stable if it does not fall. When a body is unlikely to be upset by a small movement, we say that the body is stable.
2. Unstable Equilibrium: A body moves further away from its equilibrium position when slightly displaced. The body does regain its original position.
3. Neutral Equilibrium: A body comes to rest in its new position. For example, when an object like a cylinder is pushed to the ground. The center of gravity of that cylinder does not change.

## Equilibrium of Bodies in Liquids

When you carry a bucket that is filled with water, you will definitely feel the effect of its weight. However, when you pull the same bucket with an exact quantity of water from a well. You will realize that it is not as heavy as it was in the air.

The lightness of the bucket while in the water is due to a force that pushes the bucket in an upward direction. The force will try to cancel the weight of the object that is pushing it downward. The force is called upward force or upthrust.

### Upthrust

When a body is fully or not entirely immersed in a liquid, it will face an ascending force. We can also define an upthrust as the reaction force exerted on a body when wholly or partially immersed in a fluid.

If the weight of the bucket in air is W2, and the weight of the bucket while immersed in the water is W1. Then, the upthrust on the bucket is

Upthrust, U = Weight in air (W2)  — Weight in the water (W1)

Additionally, we can find the weight when immersed in the water by making W1 subject of the formula in the above equation

Weight in the water (W1) = Weight in air (W2) — Upthrust, U

We can also apply the following formula to calculate the upthrust of an object:

Upthrust = volume of the object x density of the liquid x gravitational acceleration

Upthrust  = (V/3) x density of liquid x g

### Archimedes Principle

Archimedes’ principle states that when a body is partially or wholly immersed in a fluid, the upthrust on the body is equal to the displaced weight of the liquid.

Upthrust  = Displaced weight of the liquid

And the above expression will give us

Upthrust = volume of the object (v) x density of the liquid (ρ) x gravitational acceleration (g)

Therefore, the upthrust is

Upthrust = vρg

### Principle of Floatation

The principle of floatation states that when a body is totally or partially immersed in a fluid, its weight is equal to the weight of the displaced fluid. Examples of bodies that float are ships and ice.

Density and shape are some of the important factors that will help the body to float.

Weight of the body floating = weight of the displaced fluid

### Calculations for Equilibrium of Forces

Here are a few calculations of the equilibrium of forces to improve your understanding of the topic:

#### Problem 1

Two forces of 5 newtons each are inclined at an angle of 120 to each other. Find the single force that will:

1. Replace the given force system
2. Balance the given force system

Data

Two forces are equal = F1 and F2 = 5 N

Angle,θ = 1200

Formula

To find the single force that will replace the given force system, we will apply the formula

R2 = F12 + F22 + 2F1F2Cosθ

##### Solution

We can insert our data into the formula to solve the problem

R2 = 52 + 52 + 2 x 5 x 5 x Cos1200 = 25 + 25 + 20 x (- cos600)

We can now rewrite the above expression as

R2 = 50 – 20 x 0.5 = 50 – 10 = 40

Hence, R = √40 = 6.32 N which can be approximated to 6 Newtons

Therefore, the resultant force is 6 N.

R = 6 n

We can now apply the sign rule to obtain α

(6/sinα) = (R/sin600) = (6/sin600)

This is now equal to

Rsinα = 6sin600

This implies that

6sinα = 6sin600

and we have

sinα = sin600

which can be written as

α = sin-1 [sin600]

Therefore,

α = 600

b. Equilibrant = 6 N

#### Problem 2

A meter rule is pivoted at its midpoint C with a vertical force of 10 newtons hanging from a distance of 30 centimeters from C. At what distance must a 15 Newton force hang to balance the ruler horizontally?

Data

Vertical force, F1 = 10 N

Distance from the side of F1, S1 = 30 cm

Force on the other side, F2 = 15 N

Unknown value

Distance on the same side of F2, S2 = ? (we can use S2 to find the unknown)

Formula

The formula we need to apply is

F1S1 = F2S2

##### Solution

10 x 30 = 15 x S2

we can now make S2 subject of the formula

S2 = 300/15 = 20 cm

#### Problem 3

A boy of mass 10.0 kilograms sits at a distance of 1.5 meters from the pivot of a seesaw. If another boy of mass 20.0 kilograms sits at a distance of 1.0 meters from the pivot, will the seesaw balance horizontally?

Solution

Moment at 10 kg = 100 N

The moment of 100 N force about C = 100 x 1.5 = 150 N

Moment at 20 kg = 200 N

The moment of 200 N force = 200 x 1 = 200 N

The seesaw will tilt in the direction of the 20 kg boy.

#### Problem 3

A piece of cork density 0.25 x 103 kilograms per meter cube floats in a liquid of density 1.25 x 105 kgm-3, what fraction of the volume of the cork will be immersed? [GCE]

Solution

Total volume of the cork = V1

The volume of the submerged cork = V2

Initial density at V1 = 0.25 x 103 kgm-3

Final density at V2 = 1.25 x 105 kgm-3

Mass of the cork = volume x density

Thus

V1 x 0.25 x 103 = V2 x 1.25 x 105

To find the ratio, we say

V1/V2 = (0.25 x 103)/(1.25 x 105)

Hence

V1/V2 = 1/5 = 0.2

You may also like to read:

How to Calculate the Relative Density of a Liquid

How to Calculate the Resultant of Two Forces at an Angle