“…For the reason of simplicity, the notations , f ( u ( x , t ), t ), λ ( x , t ), γ ( t ), ϕ a ( t , p , u ), g 1 ( u , x , t , p , y ), g 2 ( u , x , t , p , y ), h 1 ( y , p ), h 2 ( y , p ), y ( t ), and ξ ( t , p , u ) are shortly denoted by , u , f , λ , γ , ϕ a , g 1 , g 2 , h 1 , h 2 , y , and ξ , respectively, except in some special cases. The cumbersome and formal calculations of the first variation, which are already presented in other publications,() are moved to Appendix A. The variations of Lagrangian functional with respect to the variations of all possible directions δ u ( x , t ), , δ y ( t ), δ α i ( x ), and δ p are written under the form of the Gâteaux derivative of .…”