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Work by Variable Force

Jun 8, 2025

Overview

This lecture covers how to calculate the work done by a general variable force, extending techniques beyond the special case of spring forces.

Calculating Work for Variable Forces

  • For a general variable force in one dimension, calculate work by integrating force over displacement.
  • The work equals the area under the curve of a force vs. position graph.
  • When the force is constant in a small interval, work is force times displacement for that segment.
  • Summing (integrating) all these small segments as their width approaches zero gives total work.
  • Mathematically, total work ( W = \int_{x_i}^{x_f} F(x) dx ), integrating force from initial to final position.
  • In three dimensions, integrate each component of the force over its respective displacement._

Work-Kinetic Energy Theorem

  • The work-kinetic energy theorem still applies for variable forces: work equals the change in kinetic energy.
  • Once work is found (via integration or area under curve), use it to determine kinetic energy change.

Applications and Techniques

  • For known force vs. position relationships, you can integrate analytically or, if possible, graphically.
  • Graphical methods involve calculating the literal area under the force-position curve.
  • This method is less common than using constant-force equations but is essential for more complex problems.

Key Terms & Definitions

  • Variable Force — A force whose magnitude or direction changes with position.
  • Integration — Mathematical process of summing infinitesimal contributions, used here to calculate work.
  • Work-Kinetic Energy Theorem — States that the net work done on an object equals its change in kinetic energy.
  • Area under the Curve — Represents total work done when plotting force against position.

Action Items / Next Steps

  • Practice integrating variable force functions to find work.
  • Use graphical analysis for work calculation when force is given as a graph.
  • Review the work-kinetic energy theorem for both constant and variable forces.