I was also searching for similar article but there is none. We have to speculate. If we consider maximum effect, that is, application of the formula as it is, at 1 mm distance (maximum insulation thickness) then we can go on reducing it linearly (we assume infinite length that is very long conductor). In short, losses due to second term will have to be multiplied by 1x1/d or f=1/d, where d is the radial thickness of the duct in mm. Let there be S sections made by cooling ducts. Then apply second term only to one section. If these losses are W then actual loss will be W(1+f); for all cases when f is less than or equal to 1. Total eddy loss due to proximity will be S*W(1+f). This loss should then be added to first term loss to get total eddy current loss. I think this will work with sufficient accuracy.
Normally number of radial strips are low in layer winding but high in disc winding. It would be interesting to find out effect on losses due to introduction of duct of large thickness (10 mm).