The question is kind of backwards
The reason you need LDA+U in DFT is that there are no fitting parameters to get e.g. the bandgap right. However, in Huckel we have no such problem - since we do have fitting parameters. So, there is no real point to fit the Huckel model to LDA+U - just fit it to experiments (or GW or similar)!
Of course, if you have a particular reason to, say, compare an EHT calculation with an LDA+U calculation, then, perhaps... But otherwise I don't really see any compelling reason for intermixing LDA+U and EHT.
The point is rather, how transferable the EHT parameters are. The fitted parameters might only work well for a subset of problems, while DFT is a much more generic. However, as soon as you introduce LDA+U you again fit, and thus restrict things. In both cases (EHT/LDA+U) the hope is naturally that you can go a little bit, or a lot, outside of the configuration space in which you fitted, and hopefully the parameters don't change too much.
Taking something like ZrB2 as an example, we have EHT parameters for Zr, and for B, but that doesn't necessarily (or rather probably!) work for ZrB2. So you'd want to do a fit for Zr and B in ZrB2, but again the reference is best chosen as something like GW or experiments.