For an arclength-parametrized curve define the Frenet frame by , , and . Differentiating the unit lengths gives diagonal frame-derivative coefficients zero. Also implies , while . Define the torsion of a space curve by . Orthogonality then gives
These are the Frenet formulae. Differentiating also verifies the chosen torsion sign; equivalently .
At a fixed initial parameter choose an orthogonal map sending to , to and to . Its determinant is . The transformed curve has Frenet frame , so its curvature is and its torsion is .
Both its frame and the frame of solve the same linear Frenet system with the same initial data. The uniqueness theorem for a linear ordinary differential system with continuous coefficients makes the frames identical on the whole interval. In particular , so their difference is a constant vector . Thus
The orientation-reversing rigid motion accounts for the reversal of torsion.
For the positively oriented simple closed boundary, the turning tangent theorem gives . If is its length, continuity gives a point with . The planar isoperimetric inequality gives , hence
For the reversed orientation the curvature integral is , so a point of nonpositive curvature already proves the stated positive upper bound. The region-bounding interpretation is the ordinary Jordan-curve one; self-intersections would require specifying a different notion of enclosed area.

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