“…We can give intrinsic proof of the direct part of Theorem 3 (see, e.g., [55]). Recall first that in the geometric approach to Lagrangian mechanics, we have summarised in Section 5 when one starts with a 1-dimensional configuration space, Q ≡ R, and hence, TQ ≡ R × R, and the expressions of S and θ L in local coordinates (q, v) are…”