The Schrodinger Equation in a Classical Context: Superconductivity: Feynman's Physics Explained

Feynman Vol III11-12

Superconductivity is a spectacular, large-scale quantum effect. Below a critical temperature, some metals lose all electrical resistance and expel magnetic fields entirely. The reason is that electrons join into 'Cooper pairs' that behave like bosons and condense together into a single quantum state described by one wave function spread across the whole wire. This large-scale quantum coherence is what gives superconductors their strange, wonderful properties.

The big idea

In a superconductor, countless electrons act as one giant quantum wave.

Think about it

How can a quantum effect, usually hidden in the tiniest particles, show up across an entire wire you can hold in your hand?

← 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