The Lagrangian in generalized coordinates 1 2 L(0, 4, 8, 4) = gm R cos(0) + − m R² (¿² sin² (0) + Ö²) - 2 (b) The generalized momenta are Pe=0m R² P₁ = m R² 4 sin²(0) (c) The Hamiltonian is CSC csc² (0) p² + P² H(0, 4, Po, P4)= - gm R cos(0) 2m R²
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