The highlighted answer says that solutions to the E&M wave equations exist that don't go at $c$. Technically, the wave equation permits solutions that don't have a 1-way speed $c$, but these solutions must time evolve in some other way to compensate. Put mathematically, if we posit a solution to the wave equation $$f_{xx} - \frac{1}{c^2}f_{tt}$$ of the form $f(x-vt)$, we find $$f'' - \frac{v^2}{c^2}f'' = 0$$ I.e. $v=\pm c$. If you want a standing wave, or a wave moving at velocity $v \neq c$, you need a solution of the following form: $$f(x,t) = g(x\pm v)h(t)$$ Then the wave equation becomes $(c^2-v^2)f''g + (c^2-1)fg'' - 2(c^2-v)f'g' = 0$, so that gives you a new set of constraints to follow.
If regular waves of the form $f(x\pm vt)$ traveled at different speeds in different directions, you'd get some strange stuff. For example, if the speed of light in one direction were $c_1$ and in the other were $c_2$, the (1D) wave equation for $\mathbf{E}$ would become $$(\partial_t - c_1\partial_x)\cdot (\partial_t - c_2 \partial_x)\mathbf{E}=0$$ The same thing holds for $\mathbf{B}$. If you work back from this to modify Maxwell's equations, this suggests a bunch of whacky stuff (as far as I can tell), including stationary electric fields generating stationary magnetic fields (or perhaps the reverse, I don't think you can fully determine this from the wave equations alone).
TLDR; as far as I can tell, Maxwell's equations fully require that the one way speed of light is the same in both directions in any reference frame. This (plus experimental issues related to the Aether) is why 19th physicists came up with what would become special relativity in the first place. I hope someone comes along to read this and correct me if I've said anything wrong.