Alternative symmetries for the Maxwell Lagrangian? I'm wondering about how to show that $A_a\rightarrow A_a+\alpha\partial_0A_a$, with $\alpha$ infinitesimal, is an infinitesimal symmetry of $\mathcal L=-\frac14F_{ab}F^{ab}$.
\begin{equation}
F_{ab}\rightarrow F_{ab}+\partial_a(\alpha\partial_0A_b)-\partial_b(\alpha\partial_0A_a)=F_{ab}+\partial_0(\alpha F_{ab}).
\end{equation}
\begin{equation}
\Rightarrow \mathcal L\rightarrow\mathcal L-\frac12F_{ab}\partial_0(\alpha F^{ab})=\mathcal L-\frac14\partial_0(\alpha F_{ab}F^{ab}).
\end{equation}
We require $\delta\mathcal L=0$ for it to be called "a symmetry of $\mathcal L$", right? Or do we only require $\delta\mathcal L=$ a total derivative? Either way, I don't seem to get what we want.
 A: We may approach the problem via differential forms, or ordinary tensor calculus:


*

*Differential Forms: The field strength tensor $F$ is a differential form given by the exterior derivative of the 1-form $A$, i.e. $F=\mathrm{d}A$ which in components is $\partial_{[\mu}A_{\nu]}$. To add a total derivative to the form $A$ is equivalent to adding the exterior derivative of a 0-form, i.e. $A \to A + \mathrm{d}\alpha$. But the new $F' = \mathrm{d}(A + \mathrm{d}\alpha) = \mathrm{d}A$ because $\mathrm{d}^2\alpha=0$. So it is a symmetry.

*Tensor Calculus: The field strength tensor is given by $F_{\mu\nu}=\partial_\mu A_\nu - \partial_\nu A_\mu$. Consider now a change of $A$, i.e. $A_\nu \to A_\nu + \partial_{\nu} \alpha$. When we plug this into the field strength tensor, we obtain $F'_{\mu \nu} = \partial_{\mu}(A_\nu + \partial_{\nu} \alpha) - \partial_\nu (A_\mu + \partial_{\mu} \alpha) = \partial_\mu A_\nu - \partial_\nu A_\mu$ because $\partial_\mu \partial_\nu \alpha = \partial_\nu \partial_\mu \alpha$, and hence the terms cancel in the expression for $F'_{\mu \nu}$.

A: Comments to the question (v2): 
It seems that OP assumes that $\alpha$ is independent of $x$, i.e., OP considers a global quasisymmetry 
$$\delta A_{\mu}=\alpha \dot{A}_{\mu}.$$ 
The corresponding conserved quantity is energy, cf. Example 1 on the Wikipedia page for Noether's (first) theorem.
