Differentiation givesThe angles ϕ and ψ are cyclic, so their canonical momenta are conserved. The Lagrangian is autonomous, so the total energy is also conserved. The momentum pθ is not generally constant because gravity and the angular kinetic terms depend on θ.
pθ=I1θ˙,pψ=I3(ψ˙+ϕ˙cosθ),pϕ=I1ϕ˙sin2θ+pψcosθ.
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