As I suspected, a rigorous mathematical examination of a circuit with a distributed load is far from trivial, but I’ve tackled ‘stage 1’.
With a bit of effort I have now satisfied myself that if one has a 32A circuit (ring or radial) with a 20A load at the furthest point, and the other 12A evenly distributed along the length of the circuit (equally in the two arms, in the case of a ring), and IF one assumes that the cable’s resistivity (mΩ/A/m) is the same throughout the cable, then the VD at the furthest point will be the same as one would calculate assuming a 26A load at the furthest point.
However, in the real world, the answer one gets by that calculation may not (I haven’t satisfied myself about this yet) be precisely correct, since current flow (hence temperature, hence conductor resistivity) will be different at every point in the cable. Not only that, but the current (hence corresponding temperature and resistivity) will rise to the ‘full’ 32A (or 2 x 16A for a ring), rather than the ‘quasi design current’ of 26A, very close to the origin of the circuit. Half of the cable length will be carrying a current greater than the 26A ‘quasi design current’, so half of the cable will have a resistivity (hence contribution to total VD) higher than that one would expect if 26A were flowing through the whole length of the cable, but the other half will be carrying less than 26A, hence lower temp/resistivity and less contribution to total VD than would be expected with a current of 26A flowing through the entire length of the cable. It remains for me to try to work out whether these two things exactly ‘cancel’....
... I suspect they may not cancel, since current varies in a linear fashion along the cable, but power dissipated, hence temperature, is presumably related to I² - so that the increased heating (hence increased VD contribution) in the more upstream parts of the circuit is probably less than the decreased heating (hence decreased VD contribution) in the more upstream parts. Watch this space.
Kind Regards, John