Science by Katharine

"What's the go of that?" – James Clerk Maxwell

If you’ve had multivariable calculus or introductory electromagnetism or fluid mechanics you’ve learned the very useful fact that the divergence of a curl is always zero: βˆ‡β‹…(βˆ‡Γ—π…)=𝟎\nabla\cdot\left(\nabla\times {\bf F}\right)={\bf 0}. Checking this identity is a straightforward calculation, but why does this work?

The identity isn’t a mathematical accident from lucky cancellations: it’s a necessary consequence of Stokes’ Theorem and the Divergence theorem working together. Here’s how to see it in pictures.

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