An Introduction to Knot Theory

Published on July 18, 2025

Explore the mathematical study of knots and their properties, a field with surprising applications.

What is a Mathematical Knot?

When we think of a knot, we usually picture a tangled piece of string with two loose ends. In mathematics, however, a knot is something more specific: it's a closed loop in three-dimensional space that doesn't intersect itself. Imagine taking a piece of string, tangling it up, and then fusing the two ends together seamlessly. The result is a mathematical knot.

The simplest knot of all is just a plain, un-knotted circle, which mathematicians appropriately call the unknot. But from there, the complexity blossoms into an infinite family of fascinating and intricate shapes.


The Central Question: Are Two Knots the Same?

The fundamental challenge in knot theory is determining when two knots are equivalent. Two knots are considered the same if one can be smoothly deformed into the other without cutting the string or allowing it to pass through itself. This concept of smooth deformation is called ambient isotopy.

To formalize this, mathematicians use a set of three fundamental transformations called the Reidemeister moves. Any deformation of a knot can be broken down into a sequence of these three moves. If you can get from one knot to another using only these moves, they are equivalent.


Knot Invariants: The Tools of the Trade

Proving two knots are the same can be done by finding a sequence of Reidemeister moves. But how do you prove two knots are different? You need to find a property that is preserved under all three moves—a knot invariant.

If two knots have a different value for a specific invariant, they cannot be the same. Some key invariants include:


Surprising Applications

While it may seem like an abstract puzzle, knot theory has profound applications in the real world.

Knot theory is a perfect example of how the study of pure, abstract mathematics can lead to deep insights into the structure of our physical world.