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The Simplest Truly Spatial Motion Hans-Peter Schröcker1 Bert Jüttler2 1 Unit Geometry and CAD Universität Innsbruck 2 Institute of Applied Geometry Johannes Kepler University Linz Conference on Geometry: Theory and Applications Pilsen, June 29 2009 Overview Dual quaternion representation Fundamental properties Biarc motion interpolation Dual quaternion cross-ratios Simplest coordinatization of the motion group Requirements • bilinear composition law • minimal number of parameters Simplest coordinatization of the motion group Requirements • bilinear composition law • minimal number of parameters Solution (Study, ≈ 1890) • dual quaternions X + εY with X, Y ∈ H and ε2 = 0 • composition law ≈ dual quaternion multiplication • essentially unique (a0 , a) 7→ (εX) ? (a0 , a) ? (X + εY)−1 with kXk2 = 1, XT Y = 0 Simplest coordinatization of the motion group Requirements • bilinear composition law • minimal number of parameters Solution (Study, ≈ 1890) • dual quaternions X + εY with X, Y ∈ H and ε2 = 0 • composition law ≈ dual quaternion multiplication • essentially unique (a0 , a) 7→ (εX) ? (a0 , a) ? (X + εY)−1 with kXk2 = 1, XT Y = 0 Euclidean displacements ⇐⇒ points (X, Y) on Study quadric S ⊂ P7 : XT Y = 0 (and X 6= 0) The simplest motions straight lines ⊂ S ⇐⇒ • rotations about fixed axis or • translations in fixed direction The simplest motions straight lines ⊂ S ⇐⇒ conics ⊂ S • rotations about fixed axis or • translations in fixed direction ⇐⇒ coupler motions of Bennett linkages Fundamental properties Line-symmetric motion • The Bennett motion is line-symmetric with respect to one family of rulings on a hyperboloid (Krames 1937). Inverse and dual motion • The inverse motion (fixed and moving frame interchanged) and the dual motion (transformation of planes) are Bennett motions. Instantaneous screws • The instantaneous screws of a Bennett motion are always of the same chirality (Baker, 1998). • The tangents of a planar section of a quadric Q always lie on the same side of Q. Trajectories Trajectories of points • (a0 , a) 7→ (εX) ? (a0 , a) ? (X + εY)−1 • rational curves of degree four Trajectories of planes • (u0 , u) 7→ (εX) ? (u0 , u) ? (X + εY)−1 • rational torses of class four Trajectories of lines • (X − εY) ? (p + εq) ? ((x0 , −x) − ε(y0 , −y)) • rational ruled surfaces of degree four Biarcs on quadrics Biarcs on quadrics (proof) J • unique rotation such that (A, a) 7→ (B, b) B b a • equal blue angles (red angles) (for reasons of symmetry) A • equal angles at A and B (by construction) • proof remains valid in the elliptic plane (Fuhs, Stachel 1988) =⇒ biarcs on oval quadrics • proof remains valid (with restrictions) in the hyperbolic plane =⇒ biarcs on ring quadrics. • computational proofs by Wang and Barry (1997) or Pottman and Wallner (2001) Bennett biarc motions Properties of Bennett biarc motions • constant chirality of instantaneous screw • simple collision tests (equations of degree four): I moving point vs. fixed plane I moving plane vs. fixed point I moving line vs. fixed line • possible joint poses form a Bennett motion • simple bi-invariant choice of joint pose is possible H.-P. Schröcker, B. Jüttler Motion interpolation with Bennett biarcs Proceedings of Computational Kinematics, Springer 2009 Dual quaternion cross-ratios (preliminary results) Cross-ratio for dual quaternions CR(A, B, C, D) = (A − B) ? (B − C)−1 ? (C − D) ? (D − A)−1 Three poses A, B, C on a Bennett motion B • In general there exists exactly one D ∈ B such that the cross-ratio is scalar: CR(A, B, C, D) ∈ R + εR. • The cross-ratio is scalar for all poses D ∈ B if B is line-symmetric with respect to an equilateral hyperboloid: 1 1 1 + 2 − 2 = 0. 2 a b c Conclusion The simplest truly spatial motion lends itself to • biarc motion interpolation and • basic collision tests. Particular features are • constant chirality during the motion and • low-degree trajectories of points, lines and planes. Future research Interpretation of dual quaternion cross-ratio: • scalar cross-ratio • cross-ratio with real norm