Laplace (1799a) showed that a particle constrained to move on a surface but otherwise subject to no forces moves along a geodesic for that surface. Thus, Clairaut's relation is just a consequence of conservation of angular momentum for a particle on a surface of revolution. Laplace, P. S. (1829) [1799a]. "Book 1, §8.". Treatise on Celestial Mechanics. Vol. 1. Translated by Bowditch, N. Boston: Hillard, Gray, Little, & Wilkins. OCLC1294937.
Laplace (1799a) showed that a particle constrained to move on a surface but otherwise subject to no forces moves along a geodesic for that surface. Thus, Clairaut's relation is just a consequence of conservation of angular momentum for a particle on a surface of revolution. Laplace, P. S. (1829) [1799a]. "Book 1, §8.". Treatise on Celestial Mechanics. Vol. 1. Translated by Bowditch, N. Boston: Hillard, Gray, Little, & Wilkins. OCLC1294937.