The Lagrangian remains invariant under the addition of an arbitrary function of time because the equations of motion are unaffected by such additions, specifically when the function is a total time derivative. This is due to the Euler-Lagrange equations relying solely on derivatives with respect to position and velocity, rendering the added function's partial derivatives irrelevant. The discussion highlights the foundational role of this invariance in advanced concepts like contact transformations and Hamilton-Jacobi theory. By identifying suitable functions and variable changes, complex classical physics problems can be simplified significantly. Understanding this principle is crucial for deeper insights into classical mechanics.