proposition 29.11 Angular velocity in Euler angles

open in the book · parts/03-classical-mechanics/12-rigid-body-rotating-frames.tex:283 · p. 980

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proposition 29.11: Angular velocity in Euler angles29.11definition 29.4: Angular velocity29.4notation 29.9: The z–x–z Euler angles used in this treatise29.9definition 29.35: The Lagrange top29.35remark 29.12: The coordinate singularity, and what it is not29.12proof : ch:12-rigid-body-rotating-frames@proof-7proofdefinition 14.26: The rotation group14.26lemma 14.62: The Levi-Civita symbol is invariant14.62proposition 14.27: Generators of so(3)14.27proposition 29.5: The velocity field of a rigid body29.5theorem 29.7: Transport theorem29.7theorem 29.3: Euler's rotation theorem29.3remark 29.10: Other conventions, and why the choice must be stated29.10definition 21.31: Lagrangian21.31theorem 29.16: Principal axes29.16proposition 14.31: SO(3,ℝ) is not simply connected14.31

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typedirectionnode provenancewhere
depends_on Angular velocity declared parts/03-classical-mechanics/12-rigid-body-rotating-frames.tex:295
depends_on The $z$–$x$–$z$ Euler angles used in this treatise declared parts/03-classical-mechanics/12-rigid-body-rotating-frames.tex:295
depends_on The Lagrange top declared parts/03-classical-mechanics/12-rigid-body-rotating-frames.tex:1248
depends_on The coordinate singularity, and what it is not declared parts/03-classical-mechanics/12-rigid-body-rotating-frames.tex:345
proves ch:12-rigid-body-rotating-frames@proof-7 declared parts/03-classical-mechanics/12-rigid-body-rotating-frames.tex:298