In Noether's theorem, what is a "classical solution of the equations of motion"? I'm reading a book which states that:

for each generator of a global symmetry transformation, there is a
  current $j^{\mu}_{a}$ which, when evaluated on a classical solution
  of the equations of motion $\phi_{cl}$, is conserved. I.e.
  $\partial_{\mu}j^{\mu}_{a}\vert_{\phi=\phi_{cl}} =0 $

I get the general principle, but I'm uncertain about the bit I have made italics. Can anyone shed some light on this?
 A: 1) The word classical in this context means $\hbar=0$. 
2) In the context of an action principle, the Euler-Lagrange equations 
$$ \frac{\delta S}{\delta\phi^{\alpha}}~\approx~0 $$
are often referred to as the (classical) equations of motion (eom), cf. comment by Jia Yiyang. Here the $\approx$ symbol means equality modulo eom.
Let on-shell (off-shell) refer to whether eom are satisfied (not necessarily satisfied), respectively. 
3) In the context of a global continuous (off-shell) symmetry of an action, Noether's (first) theorem implies an off-shell Noether identity 
$$d_{\mu} J^{\mu} ~\equiv~ - \frac{\delta S}{\delta\phi^{\alpha}} Y_0^{\alpha},$$ 
where $J^{\mu}$ is the full Noether current, and $Y_0^{\alpha}$ is a (vertical) symmetry generator.
This leads to an on-shell conservation law 
$$d_{\mu} J^{\mu}~\approx~0.$$
A: The classical equation of motion can be find solving the Euler-Lagrange equation for the Lagrangian of the system $L=L(q,\dot{q})$, then EL equation states $$\frac{\partial L}{\partial q_i}-\frac{\text{d}}{\text{d}t}\frac{\partial L}{\partial\dot{q}_i},\text{  }i=1,\dots,n.$$
The conserved current $j_a^\mu$ come from the fact that if a system has a symmetry then something linked with the symmetry is kept by the system. If a system show a time symmetry then the Energy must be conserved, if a system show a traslational symmetry then linear momentum must be conserved and if a system has a rotational symmetry then angolar momentum must be conserved.
