Use the Levi-Civita symbol and the contraction of two Levi-Civita symbols in Cartesian coordinates. With repeated indices summed,The last line is the product rule. Reading its four terms in vector notation proves the curl of a cross product identity:
For an oriented piecewise smooth surface with boundary curve , and a continuously differentiable vector field near , Stokes theorem statesHere is the chosen unit normal, is positive surface area, and is the directed tangent line element. The positive traversal of is fixed by the right-hand rule relative to . Thus the flux of the curl through the surface equals the circulation along its oriented boundary.
Differentiate the position vector, keeping the other coordinates fixed in each derivative:The first two have zero dot product, since their two planar contributions cancel, and both are orthogonal to . Hence these are orthogonal coordinates away from coordinate degeneracies. Their scale factors, which are the lengths of these coordinate basis vectors, areFor example . The unit basis vectors are when ; the given coordinate basis vectors themselves are not normalized. The Jacobian determinant is except on the focal lines. These are elliptic cylindrical coordinates.
For , eliminating givesThus constant surfaces are confocal elliptic cylinders parallel to the axis. The limiting surface is the vertical strip , .
For generic , eliminating givesThese are hyperbolic cylinders with the same focal lines. A specified angular value selects the half-branch with and , because . At the surfaces are the vertical half-planes , or ; at they are , or .
Finally, constant gives horizontal planes. The three surface families express the orthogonality of elliptic cylindrical coordinates.
The ellipse bounding the surface is . With the upward normal, its positively oriented boundary is traversed by increasing from zero to :The given components are Cartesian components, so their ordinary dot product with this tangent isTherefore Stokes theorem givesA direct check uses and , hence , and multiplies by the ellipse area . The third component cannot affect either calculation because the surface and its boundary lie at fixed . Equivalently one may apply Stokes to the smooth planar field , avoiding any need to differentiate the elliptic-coordinate expression for the third component at its foci.
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