Often, in theoretical physics you hear things like "the coupling constants depend on the energy scale". One random example:
When this dependence on the scale is studied carefully, we find out that the dimensionless constants such as the fine-structure constant aren't really dimensionless, or aren't really constant. They run – depend on the energy – in a slower way and this running is the reason why the limit is singular if we want the theory to work at arbitrarily high energies or short distance scales.
But how is this even possible? The energy should not appear in the Lagrangian or equations of motion (EOM): it is a property of solutions to the EOM. Consider for example the wave equation, $$\frac{1}{v^2}\frac{\partial^2u}{\partial t^2}-\frac{\partial^2u}{\partial t^2}=0.$$ I feel like this quote would be equivalent to saying that $v$ depends on energy, i.e. $v=v(E)=v(E(u(x,t))$. This would mean the couplings depend in some complicated (and nonlinear!) way on the fields themselves. So how does this work in QFT?