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Geodesic triangles need not have Euclidean angle sum
Statement
False: every geodesic triangle on every Riemannian surface has angle sum . The unit round sphere carries a geodesic triangle with three right angles, so the flat angle sum fails there; a spherical octant has angle sum .
Facts & Assumptions
Given: The claim that a geodesic triangle on every Riemannian surface has angle sum , to be refuted by one explicit geodesic triangle.
For with the round metric induced by the Euclidean inner product, every constant-speed parametrization of a great circle is an affinely parametrized geodesic, and conversely every nonconstant affinely parametrized geodesic has a great-circle arc as its image (Great circles as round-sphere geodesics).
The Euclidean inclusion of induces its round metric; in particular for tangent vectors at a point of the round inner product is the ambient Euclidean inner product , so intrinsic angles of tangent vectors equal their ambient angles (The round metric on the sphere as an induced metric).
Assuming the axiom of choice (The Axiom of Choice), for a positively oriented compact regular disk region with exactly three vertices whose boundary is the cyclic concatenation of three regular geodesic segments with non-antipodal one-sided tangents, and which lies in a frameable neighbourhood, where are the interior sector angles (Gauss-Bonnet for a geodesic triangle).
Refutation
Let be the standard orthonormal basis of and set in the unit round sphere. Its boundary is the cyclic concatenation of the three great-circle arcs , and , , which meet only at the distinct vertices . Each is a constant-speed parametrization of a great circle with speed , so by [F1] each is an affinely parametrized geodesic; the one-sided unit tangents at every vertex are distinct non-antipodal orthonormal vectors.
At the vertex the two directions into along the boundary arcs are the ambient vectors and : the arc leaves with velocity , and the arc approaches with velocity , so its direction toward is . The same holds cyclically: the directions into at are and , and at they are and . Each listed pair is orthonormal in the ambient inner product and lies in the tangent space at the corresponding vertex, so by [F2] each interior sector angle of is .
By steps 1.1 and 1.2 the three interior angles of the octant are equal to , so their sum is , which differs from . This single geodesic triangle therefore refutes the asserted universal angle sum.
For the additional curvature check, assume AC as in [F3]. The map identifies with the closed planar simplex of nonnegative coordinates summing to , with inverse ; thus is a regular disk with the three ordinary corners already computed. It lies in the open hemisphere , which has one smooth coordinate chart; orthonormalizing its coordinate frame supplies a positive frame. Give the ambient orientation. The true local formula [F3] then reads ; the nonzero curvature integral is exactly the obstruction to the flat angle sum. The refutation in steps 1.1–2.1 uses only a single explicit triangle and no choice principle; this supplementary invocation of [F3] inherits its AC assumption.
Source locator
Lee, Riemannian Manifolds: An Introduction to Curvature, Chapter 9, printed pp. 156-172, states and proves the local Gauss-Bonnet formula and notes the spherical case of positive curvature in which angle sums exceed ; Datar, Lectures on Riemannian Geometry, Lecture 2, Theorem 2.0.1, printed pp. 10-13, states the same formula. The great-circle geodesics and the induced round metric used in the computation are the published library items Great circles as round-sphere geodesics and The round metric on the sphere as an induced metric; the right-angle count is computed directly here from orthonormality of the ambient basis vectors.
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Sources
- John M. Lee, Riemannian Manifolds: An Introduction to Curvature (1997) (standard reference, not scraped)
- Ved Datar, Lectures on Riemannian Geometry (standard reference, not scraped)