Work, Energy, and Power
Syllabus Unit: Mechanics
Why it matters
Chapter overview
This topic threads one idea through four subtopics: energy transfer via a force acting over a displacement. It covers when work is positive, negative or zero, how kinetic and potential energy are defined and computed, how the work-energy theorem and power connect force to motion and time, and how mechanical energy is conserved whenever only conservative forces act.
1Work Done by a Force
Work is done only when a force produces displacement along its own direction — pushing hard against a wall that doesn't move does zero physics-work, however tired you get.
Learning Objectives
- Define work done by a constant force as W = Fd cosθ, and identify θ correctly in a given scenario.
- Explain when work done is positive, negative, or zero, with a real example of each.
- Compute work done as the area under a force-displacement graph for a variable force.
- State the SI unit and dimensional formula of work.
Key Terms
In everyday language 'work' means effort; in physics it means something precise — a force must actually move its point of application, and only the component of force along that motion counts.
The formula and its angle
θ is the angle between the force vector and the displacement vector, not any other reference direction — this is the single most common source of error in work calculations.
Sign of work
- Positive work (0°≤θ<90°) — force helps the motion, e.g. gravity doing work on a falling apple.
- Negative work (90°<θ≤180°) — force opposes the motion, e.g. friction on a sliding box, or gravity on a ball thrown upward.
- Zero work — force ⊥ displacement (e.g. centripetal force in circular motion, tension on a conical pendulum) or no displacement occurs at all (e.g. pushing an immovable wall).
Work by a variable force
When force varies with position, work equals the area under the Force vs displacement graph.