Many thanks Akinbo,
1. If you take these enquiries elsewhere, it would be best to clearly number all you questions so that you can collate the answers and more easily find inconsistencies.
2. Given that your examples indicate some bulk confusion (and expense; DHL to Venus and Mars does not come cheap), let's see if some low-cost bulk answers can do the job.
3. In my terms, in the tests you define: classical black/white balls, quantum positive/negative charges AND ordinary black/white buttons are isomorphic (= corresponding or similar in form or relations in so far as your specified tests are concerned).
4. I therefore know of no one who would not accept the findings that you make at your desk with ordinary black/white buttons (or similars; like Left/Right socks). So please do this "classical" test and let us have a report confirming your above conjectures.
5. We now turn to bypassing your incorrect "using spin therefore" statements at your point #2:
5a. Spin is NOT isomorphic to the 3 "classical" classes above.
5b. Spin is a typical quantum property: which is just what we want!
5c. For spin is typically perturbed when a particle interacts with a polariser.
6. Which nicely brings us to that experiment T defined 2 posts above:* with its spin-half particles for comparison with Bell (1964). For there we have a "classical" experiment (in my terms; see essay), with quantum-style perturbations of spin-half particles to boot.
* Alas Akinbo, there is no escaping experiment T; even here where we do your bidding.
7. However, and beautifully, old Malus' Law [as adapted by me to the spin-half particles that we have here; see equations (1)-(2) below] is all you need for complete understanding: remembering that T is NOT the full-monty EPR-Bohm test in Bell (1964) but is a real (executable) non-misleading test for pedagogic purposes.
8. So, BIG HINT, with you being Alice.
P(U|T, Alice) = cos2 [(1/2)(a,b)]; (1)
P(D|T, Alice) = sin2 [(1/2)(a,b)]; (2)
E(UD|T, Alice) = (1) - (2) = a.b; (3)
since +1 is typically assigned to U, -1 to D.
9. When you are clear on this (it takes a while, but re-reading my essay may help; especially re Bohr's important insight): you will note that we have not used those tricky terms in your point #3; and we invoke no "orientation inconsistencies" per your point #4.
10. Trusting the above moves us, we growing band of CLRs (convinced local realists), to much closer agreement: please do not hesitate to raise any ongoing issues.
With thanks for the opportunity to address your concerns; and with best regards; Gordon
PS: Typos corrected and this added: I therefore know of no one who would not accept the findings that you make at your desk using equations (1)-(3) to derive E(AB|T) = -a.b.