The usuall way to "half-popularly" show that the quantum mechanics formalism is not unconnected to the classical mechanics is to demonstrate a classical case as a limit of a quantum case.
The main question: Is there a way to show that macroscopic eigenmode is formed of microscopic eigenmodes superposition?
More details: Classical solution for spatial eigenmodes of vertical displacement $y=y(x)$ is:
$$ y=\sum_{n=1}^{\infty}A_n\sin \left(\frac{n\pi x}{L}\right) $$
so there must be a $n$ (regarding the string length $L$) for which is the system not sufficiently classical any more.
On the other hand, there is a superposition of elastic arrangement states (eigenmodes) of the lattice oscillations resulting in macroscopic classical motion.
Note 1: I have chosen string because of its general familiarity. I will accept an answer e.g. for longitudinal waves in 1D rod as well.
Note 2: Of course, the classical and quantum description are based on different assumptions, formalism etc. I don't expect the classical description to magically become a quantum at some point.