The prerequisite for the length of a world line to equal proper time is that the worldline must be timelike everywhere, which is tied to the object having mass. The choice of scaling factor, whether C=i or C=1, is arbitrary and does not affect the fundamental relationship. The value of c serves merely as a ratio between units of timelike and spacelike displacements, making it relatively unimportant in this context. Proper time can be more accurately described with the equation dτ=√|ds²|, though this analogy can be imprecise. Overall, understanding these concepts requires familiarity with Minkowski geometry and the underlying principles of spacetime.