remark 29.27 Euler's equations as a Lie–Poisson system

open in the book · parts/03-classical-mechanics/12-rigid-body-rotating-frames.tex:813 · p. 985

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remark 29.27: Euler's equations as a Lie–Poisson system29.27definition 24.37: Casimir function24.37definition 24.40: Lie–Poisson bracket24.40proposition 29.26: The two integrals of torque-free motion29.26definition 24.36: Poisson manifold24.36proposition 24.15: Poisson bracket from the symplectic form24.15proposition 24.41: The free rigid body is a Lie–Poisson system24.41theorem 24.38: Symplectic foliation, quoted24.38definition 5.127: Lie algebra5.127equation 29.12: eq:rigid-kinetic-energy29.12theorem 29.25: Euler's equations29.25proposition 29.33: Dissipation drives a free body to its largest moment29.33proposition 29.43: The three integrable heavy tops29.43remark 29.30: Polhode and herpolhode29.30remark 24.42: The intermediate axis24.42theorem 29.29: Poinsot's construction29.29proof : ch:12-rigid-body-rotating-frames@proof-17proof

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