(a) Using the theorem concerning Poisson brackets of vector functions and components of the angular momentum, show that if F and G are two vector functions of the coordinates and momenta only, then
(b) Let L be the total angular momentum of a rigid body with one point fixed and let Lμ, be its component along a set of Cartesian axes fixed in the rigid body. By means of part (a) find a general expression for
(Hint: Choose for F and G unit vectors along the μ and v axes.)
(c) From the Poisson bracket equations of motion for Lμ derive Euler’s equations of motion for a rigid body.
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