Work and Potential Energy (Conclusion): Feynman's Physics Explained

Feynman Vol I6-7

The power of potential energy is that it lets us use conservation of energy directly. For a conservative force — gravity, or an ideal spring — the sum of kinetic and potential energy is a constant, a result that follows straight from Newton's laws. For nonconservative forces like friction, energy is not conserved in the same simple way; it leaks away as heat. The clean test for a conservative force: the work done around any closed loop is zero, so you can never get free energy by going around in a circle.

The big idea

You can't get free energy by going in a loop.

Think about it

Why is a machine that claims to run forever with no energy input (perpetual motion) impossible?

← More Physics (Feynman Lectures) guides  ·  Explore the Physics (Feynman Lectures) module →

📧 Get a free brain-teaser every morning

Join thousands of families learning something new each day.

Subscribe free