I found that URL a while ago and was mulling over it yesterday. The closest approximation I could find was at the bottom of page 14 but they never say what "the enclosure" is and they only give you F13, not F31.
Then I found this video:
, which circumvents having to do any calculus whatsoever because 1 of the terms cancels out. In that video he uses a cylinder. Since all surfaces of the cylinder have divergent normals, the cylinder can't see itself and F22 = 0. This means F21 = 1 and via reciprocity you can find F12. In my case I'm using a hemisphere inside of a cube rather than another sphere so I have to make 2 assumptions:
Since a hemisphere also has divergent normals, F22 should also be 0, leading to the same conclusion as the video, that F12 is merely a ratio of areas between 1 and 2.
Via Nusselt, the "patch" projected by a differential area from 2 onto 1 can be instead projected onto a virtual sphere and should cover the same proportional area of the enclosure. So imagining the oven as a sphere instead of a cube, may change the patch shape and total area but shouldn't much change the patch's proportional area.
From these assumptions, A1F12 = A2F21 or F12 =A2/A1 (F21 = 1). Therefore F12 = 0.5 (4piR^2)/(4piR^2). As it turns out, this is a very very small number (0.07) for a 12 lb turkey, giving me an unsatisfactory contribution from radiation.
I am already assuming the metal surfaces are perfect black body radiators and the turkey has emmissivity of 0.8 (it's been shown that meat's emmissivity drops as it browns). I can add a fudge factor to the view factor because the meat cannot be idealized as a sphere but will always have more area than that perfect shape, but this might only buy me another 10-15% or something. I still feel like either I made a mistake or there's something missing from the radiation side.