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Geodesic triangles need not have Euclidean angle sum

Statement

False: every geodesic triangle on every Riemannian surface has angle sum π. 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 3π/2.

Facts & Assumptions

Given: The claim that a geodesic triangle on every Riemannian surface has angle sum π, to be refuted by one explicit geodesic triangle.

[F1]

For n≥1 with the round metric induced by the Euclidean inner product, every constant-speed parametrization of a great circle Sn∩span⁡{p,u} 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).

[F2]

The Euclidean inclusion of Sn induces its round metric; in particular for tangent vectors u,v at a point of S2⊂R3 the round inner product is the ambient Euclidean inner product ⟨u,v⟩, so intrinsic angles of tangent vectors equal their ambient angles (The round metric on the sphere as an induced metric).

[F3]

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 C2 geodesic segments with non-antipodal one-sided tangents, and which lies in a frameable neighbourhood, ∫TK dA=α+β+γ−π where α,β,γ are the interior sector angles (Gauss-Bonnet for a geodesic triangle).

Refutation

technique · exhibit the first-octant spherical triangle, compute its three interior angles as right angles, and compare with the flat angle sum
1.1F1given

Let e1,e2,e3 be the standard orthonormal basis of R3 and set O:=S2∩{x1≥0, x2≥0, x3≥0} in the unit round sphere. Its boundary is the cyclic concatenation of the three great-circle arcs σ1(t)=cos⁡t e1+sin⁡t e2, σ2(t)=cos⁡t e2+sin⁡t e3 and σ3(t)=cos⁡t e3+sin⁡t e1, 0≤t≤π/2, which meet only at the distinct vertices e1,e2,e3. Each σi is a constant-speed parametrization of a great circle with speed 1, so by [F1] each is an affinely parametrized geodesic; the one-sided unit tangents at every vertex are distinct non-antipodal orthonormal vectors.

1.2F2given

At the vertex e1 the two directions into O along the boundary arcs are the ambient vectors e2 and e3: the arc σ1 leaves e1 with velocity σ1′(0)=e2, and the arc σ3 approaches e1 with velocity σ3′(π/2)=−e3, so its direction toward e3 is e3. The same holds cyclically: the directions into O at e2 are e3 and e1, and at e3 they are e1 and e2. 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 O is arccos⁡0=π/2.

2.1step 1.1step 1.2algebra

By steps 1.1 and 1.2 the three interior angles of the octant O are equal to π/2, so their sum is 3π/2, which differs from π. This single geodesic triangle therefore refutes the asserted universal angle sum.

3.1F3step 1.1step 2.1algebra∎

For the additional curvature check, assume AC as in [F3]. The map x↦x/(x1+x2+x3) identifies O with the closed planar simplex of nonnegative coordinates summing to 1, with inverse u↦u/∣u∣; thus O is a regular disk with the three ordinary corners already computed. It lies in the open hemisphere x1+x2+x3>0, which has one smooth coordinate chart; orthonormalizing its coordinate frame supplies a positive frame. Give O the ambient orientation. The true local formula [F3] then reads ∫OK dA=3π/2−π=π/2; 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 π; 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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