Math 2.0

statement theorem

Stokes' theorem

Statement

Let D⊆R2D \subseteq \mathbb{R}^2 be the compact region bounded by a piecewise smooth simple closed curve γ\gamma, oriented counterclockwise. Let rr be an injective regular parametrised surface of class C2C^2 on an open set that contains DD. Let S=r(D)S = r(D) have the unit normal n=(ru×rv)/∥ru×rv∥n = (r_u \times r_v) / \| r_u \times r_v \|, and let ∂S\partial S be the closed curve r∘γr \circ \gamma. If FF is a vector field of class C1C^1 on an open set that contains SS, then ∮∂SF⋅dr=∬S(∇×F)⋅n dS.\oint_{\partial S} F \cdot d\mathbf{r} = \iint_S (\nabla \times F) \cdot n \, dS.

Remarks

The left side is the circulation of FF around the boundary. The right side is the flux of the curl of FF through SS. The orientations match by the right-hand rule: with the thumb along nn, the fingers curl in the direction of ∂S\partial S. Example: for the upper unit hemisphere and F=(−y,x,0)F = (-y, x, 0), ∇×F=(0,0,2)\nabla \times F = (0, 0, 2), and both sides equal 2π2\pi. For a flat surface in the xyxy-plane, the theorem reduces to Green's theorem. The proof pulls the integrals back to DD and applies Green's theorem there.

History

The theorem first appears in a letter from William Thomson to George Stokes in 1850. Stokes set it as a question on the Smith's Prize examination at Cambridge in 1854, and the result then got his name.

Explanations

L1 human

The total swirl of a field over a surface equals the circulation of the field around the edge of the surface. The surface can be any shape: only its boundary curve matters.

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Sources

  1. Web https://en.wikipedia.org/wiki/Stokes%27_theorem, Theorem
  2. Web https://en.wikipedia.org/wiki/Stokes%27_theorem, History