I have not assumed that the "circuit was always in the steady state". The "many others" asume that you can retain a non-steady-state accumulation after the circuit has relaxed into an Ohmic steady-state: This is unadultertaed claptrap.
No, those "many others" are not just
assuming. They are led to their conclusions by mathematics and physics. Dr Prins has been unable to refute that mathematics and physics, which is why he is repeating his baseless assertions with increasingly colorful language while touting his qualifications and attacking the qualifications of those who disagree with him.
At one point, Dr Prins claimed to have a mathematical argument in favor of
Prins's Law. That argument was demolished by several posters, including several who gave simple counterexamples to Dr Prins's mathematical arguments. In this post, I will give a quantitative version of
sol invictus's counterexample, which uses automobiles and traffic as analogies for charge carriers and current.
Dr Prins is conflating automobile density (automobiles per kilometer) with traffic density (automobiles per minute). As sol invictus pointed out, constant traffic density does not imply constant automobile density.
Suppose we have a long stretch of straight road, divided into equal thirds, with a speed limit of 120 km/h in the first third, 60 km/h in the second third, and 120 km/h in the last third. Suppose further that all traffic on this road travels at the speed limit. (That's an simplification: We're neglecting the brief periods of deceleration and acceleration that would be necessary, because taking those periods into account would complicate our calculations without changing our conclusions.)
Suppose further that automobiles are seen to enter this long stretch of road at the rate of 1 automobile every 6 seconds, and that automobiles are seen to exit this long stretch of road at exactly the same rate. Let's suppose that this 10 automobiles/minute rate of traffic is constant throughout the entire stretch of road.
Those assumptions are analogous to assuming a constant current through a sandwich of dissimilar conducting materials. According to
Prins's Law, those assumptions imply constant
charge automobile density all along the long stretch of road. As will be seen, however, assuming a constant rate of traffic implies that the automobile density within the 60 km/h section is twice the density within the 120 km/h section.
Consider the transition from 120 km/h to 60 km/h. The rate of traffic is a constant 10 automobiles per minute, so 10 cars travel through that transition every minute. Successive cars are separated by 6 seconds.
On the 120 km/h side of the transition, that 6-second separation in time implies a separation of 200 m in distance. (At 120 km/h, each car is travelling 2000 meters per minute, which is 200 meters per 6 seconds.)
On the 60 km/h side of the transition, that 6-second separation in time implies a separation of 100 m in distance. (At 60 km/h, each car is travelling 1000 meters per minute, which is 100 meters per 6 seconds.)
When the speed limits differ, a constant rate of traffic (analogous to constant current density) tells us that the automobile density (analogous to charge density) cannot be constant.
That's a simple counterexample to the mathematical arguments Dr Prins has offered in favor of his belief that constant current density implies constant charge density.
Although the automobile analogy above refutes Dr Prins's mathematical arguments quite adequately, it does not (by itself) rule out the possibility that
Prins's Law holds for a certain class of conducting materials, such as metals. Although different metals have different drift velocities (just as they have different resistivities), the charge density of conducting metals is normally very close to zero. If the charge density of conducting metals were always exactly zero, then
Prins's Law would hold for metals despite the fact that the arguments Dr Prins has advanced in support of that law have been utterly bogus.
We know, however, that the charge density within metals is not always zero. In particular, we can change the charge density within a conducting metal tube by placing it within an electric field directed perpendicular to the main axis of the tube. By the superposition principle, that gives us a clear counterexample to
Prins's Law even if the composition of the metal tube is homogeneous. Since
Prins's Law fails even for homogeneous materials, it cannot be cited as Dr Prins's sole authority when he is arguing about a sandwich of dissimilar metals.