Equilibrium of forces

When several forces act on a body, the body is said to be in equilibrium if it remains at rest or moves with constant velocity. For equilibrium, both the resultant force and the resultant moment (torque) on the body must be zero.

Principle of Moments

The principle of moments states that for a body in equilibrium, the sum of the clockwise moments about any point is equal to the sum of the anticlockwise moments about that same point.

A clean, minimalist diagram of a horizontal beam balanced on a pivot. Show two forces acting at different distances from the pivot: one force downwards on the left, another downwards on the right. Use simple arrows and label the distances and forces. Indicate clockwise and anticlockwise moments with curved arrows.

Definition

The moment of a force about a point is the product of the force and the perpendicular distance from the point to the line of action of the force.

Mathematically, for equilibrium:

(clockwise moments)=(anticlockwise moments)\sum (\text{clockwise moments}) = \sum (\text{anticlockwise moments})

Conditions for Equilibrium

A body is in equilibrium if:

  • The resultant (net) force on the body is zero.
  • The resultant (net) moment (torque) about any point is zero.

This means the body will not accelerate linearly or rotate.

Important

Both translational and rotational equilibrium must be satisfied for complete equilibrium.

Vector Triangle for Coplanar Forces

If three coplanar forces act on a body in equilibrium, they can be represented in both magnitude and direction by the sides of a closed triangle drawn to scale.

A minimalist vector triangle diagram: three arrows connected head-to-tail forming a closed triangle. Each arrow is labeled as a force (F1, F2, F3). The style is clean, with thin lines and no shading, suitable for a modern UI.

To construct the vector triangle:

  1. Draw the first force as an arrow to scale.
  2. From the head of the first arrow, draw the second force to scale.
  3. From the head of the second arrow, draw the third force to scale.
  4. The triangle should close (the third arrow ends at the tail of the first), confirming equilibrium.
Exam Tip

When drawing a vector triangle, use a ruler and protractor for accuracy, and label all forces clearly.

Example: Applying the Principle of Moments

Suppose a uniform beam is balanced horizontally on a pivot. A 20 N weight hangs 2 m from the pivot on one side, and a 10 N weight hangs 4 m from the pivot on the other side.

Calculate the moments about the pivot:

  • Clockwise moment: 20N×2m=40Nm20\,\text{N} \times 2\,\text{m} = 40\,\text{Nm}
  • Anticlockwise moment: 10N×4m=40Nm10\,\text{N} \times 4\,\text{m} = 40\,\text{Nm}

Since the moments are equal, the beam is in equilibrium.

A simple, modern illustration of a horizontal beam on a pivot. On the left, a 20 N weight hangs 2 m from the pivot; on the right, a 10 N weight hangs 4 m from the pivot. Use minimalist arrows to show forces and label all distances and weights.

1

Example

A uniform beam 3 m long is supported at its center. A 30 N weight is hung 1 m from the left end. Where should a 20 N weight be hung from the right end to balance the beam?

Summary

  • For equilibrium: net force = 0, net moment = 0.
  • The principle of moments applies to rotational equilibrium.
  • Three coplanar forces in equilibrium can be represented by a closed vector triangle.

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