Work done by a force
Work is an energy transfer. A force does mechanical work only when the point where it acts moves and the force has a component along that displacement. Begin with the direction of the displacement, not with a memorised sign.
Only the force component along the displacement does work
Definition
What is meant by mechanical work?
Model answer: The energy transferred by a force as its point of application moves through a displacement.
Symbols
- = work done by the force (J)
- = magnitude of the constant force (N)
- = magnitude of the displacement (m)
- = angle between the force and the displacement (degrees or radians)
Swipe left or right to see the whole diagram →
The angle between two directions is taken from to . One joule is the work done by a 1 N force acting through 1 m in its direction: .
- A force in the direction of motion has , so .
- A force perpendicular to the motion has , so it does no work.
- A force directly opposite the motion has , so its work is negative.
Common mistake
Separate signed work from work done against a force
The sign tells you the direction of energy transfer. A positive work term transfers energy into the chosen body or system; a negative term transfers energy out.
Worked example
A force acting at an angle
A constant 50 N force pulls a body through 5 m. The force is at to the displacement.
- “Work done by a 12 N resistance over 4 m” is J.
- “Work done against that resistance” is the positive magnitude, J.
- A person holding a stationary load may feel tired, but the force does zero mechanical work on the load because its displacement is zero.
Key idea
Calculate the work of each real force before adding
- Mark the displacement direction and distance.
- List only the real forces acting during that displacement.
- Find the angle between each force and the displacement.
- Calculate each signed work term, then add if total work is required.
On a body moving along a fixed smooth surface, the normal reaction is perpendicular to each small displacement. Its work is therefore zero.
The total work is the signed sum of the work done by the real forces.
A 40 N force pulls a box 6 m along a horizontal floor. The force acts at above the horizontal and the resistance is 8 N. Find the work done by the pulling force, the work done by resistance and the total work on the box.
