I remember seeing an explanation of this years ago which revolved around the leverage effect that stopping a rotating object causes but can’t find the article.
It basically drew a line from the axle to the tyre’s contact patch on the ground which was “lever 1” then another from the axle to the rim braking surface “lever 2” and a third from the axle to the centre point of a disc brake rotor, “lever 3”. It went on to show that the force on lever 1 (mass x velocity)needed to be counteracted to stop the bike.
Then it demonstrated that because 1 and 2 were fairly close in terms of length, the force (leverage) needed to slow the bike was slightly more than that being generated. However, because lever 3 (the disc brake) was so much shorter than 1, the actual force needed to stop was much, much greater.
The upshot was, because the ‘fulcrum point’ for all 3 was the axle and the only part of the bicycle that was connected to that was the fork, the fork itself needed to be considerably stronger and stiffer for the disc brake.
That all probably comes across as nonsense so I’ll keep looking for the article…..
Edit: Slow typing means that others have put it so much simpler 😳