It is well-known that Maxwell added the displacement current term to Ampère's Law to make electrodynamics whole. As it is taught in the modern context (I am currently reading Griffiths's text, Introduction to Electrodynamics), we can motivate the addition of the displacement current term by noting that its addition to Maxwell's equations means that Maxwell's equations imply the continuity equation. However, as Griffiths remarks, this nicety (the fact that the continuity equation falls out of Maxwell's equations) is not incontrovertible evidence that the addition of the specific form of the displacement current term is necessarily correct. Indeed, he says that there "might, after all, be other ways to doctor up Ampère's Law". My question is, therefore, twofold:
(1) Is it true, as Griffiths says, that there are conceivably other ways to "fix" Ampere's Law? That is, can we let $$\nabla \times \mathbf{B}=\mu_{0}\mathbf{J}+\mathbf{v}$$ for some arbitrary vector function $\mathbf{v}$ and still develop a consistent theory? I'm not sure how to define "a consistent theory" here but, perhaps, we can roughly say that a consistent theory would mean no contradictions with the other three Maxwell equations (mathematically-speaking). At least to me, I would suspect that the answer is "yes" since the problem (at least as it is understood in the more modern language of vector calculus, as compared to what Maxwell was doing) with Ampere's Law without Maxwell's correction is that the divergence of the right-hand side does not in general vanish, as it must. Thus we would be requiring that (using continuity and Gauss's Law) $$\nabla \cdot \mathbf{v}=-\nabla \cdot(\mu_{0}\mathbf{J})=\mu_{0}\frac{\partial\rho}{\partial t}=\mu_{0}\nabla \cdot(\epsilon_{0}\frac{\partial\mathbf{E}}{\partial t})$$ but, of course, the divergence of a vector function does not fully specify that vector function. However, assuming we choose $\mathbf{v}$ to satisfy the above, and putting aside experimental verification for the moment, would choosing something else for $\mathbf{v}$ break the structure of Maxwell's theory somewhere else?
(2) Moving now to consider experimental verification, Griffiths says that Hertz's discovery of EM waves confirmed Maxwell's choice for the displacement current term. I understand that Maxwell's equations imply wave solutions that were observed experimentally, but perhaps someone can (at a high-level, even) explain why any other choice of the displacement current term would have yielded inconsistencies with experiment (assuming that my attempt at answering (1) above was correct for, if there are mathematical inconsistencies, then we are done).