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Mancosu - Philosophy of Mathematical Practice (Oxford, 2008).pdf

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purity <strong>of</strong> method in hilbert’s grundlagen 235rotated into it. Parallel transport does not alter length, but crucially rotationsometimes does.³⁸Hilbert now considers the point (1, 0) on the x-axis, and rotates thispositively through the infinitesimal angle t. This will give a segment OA,where O is the origin and A has coordinates (x ′ , y ′ ) determined byx ′ + iy ′ = e (1+i)t · (x + iy) = e (1+i)t · x = e (1+i)tsince y = 0andx = 1. This is then:e t+it = e t · e it = e t · (cos t + isint) = e t cos t + ie t sin tgiving the coordinatesx ′ = e t cos t,y ′ = e t sin tAccording to the method <strong>of</strong> determining length, segment OA necessarily haslength 1.Now we construct the reflection <strong>of</strong> A in the x-axis, giving A ′ withcoordinates (x ′ , −y ′ ), and A and A ′ are then connected by a line perpendicularto the x-axis; denote by B the point where this line cuts the axis (Fig. 8.4).qA (x′,y′)OtB(1,0)(e 2t , 0)qA′ (x′, −y′)Fig. 8.4. The triangle showing the failure <strong>of</strong> the Isoceles Triangle Theorem.³⁸ A key part <strong>of</strong> the pro<strong>of</strong> is showing, <strong>of</strong> course, that the Congruence Axioms hold. Hilbert’s workis not explicit about this. In his new version <strong>of</strong> Appendix II to the Seventh Edition <strong>of</strong> the Grundlagen,Schmidt uses one ‘congruence mapping’ in place <strong>of</strong> the distinct notions <strong>of</strong> parallel transport androtation. This is essentially the rotation function described above, with ‘transport’ parameters added,i.e. x ′ + iy ′ = e iθ+(1+i)τ · (x + iy) + λ + iµ, whereλ, µ are taken to be elements <strong>of</strong> T. Schmidt thenproceeds to give careful verifications <strong>of</strong> the Congruence Axioms.

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