After a decade of many claims to the opposite, there now is a growing consensus that generic disordered quantum wires, e.g., the XXZ-Heisenberg chain, do not exhibit many-body localization (MBL)-at least not in a strict sense within a reasonable window of disorder values W. Specifically, computational studies of short wires exhibit an extremely slow but unmistakable flow of physical observables with increasing time and system size ("creep") that is consistently directed away from (strict) localization. Our work sheds fresh light on delocalization physics: Strong sample-to-sample fluctuations indicate the absence of a generic time scale, i.e., of a naive "clock rate"; however, the concept of an "internal clock" survives, at least in an ensemble sense. Specifically, we investigate the relaxation of the imbalance I(t) and its temporal fluctuations F(t) and the entanglement and Renyi entropies, Se(t) and S2(t), in a one-dimensional system of interacting disordered fermions. We observe that adopting Se(t), S2(t) as a measure for the internal time per sample reduces the sample-to-sample fluctuations but does not eliminate them. However, a (nearly) perfect collapse of the average I(t) and F(t) for different W is obtained when plotted against Se(t) or S2(t), indicating that the average entropy appropriately models the ensemble-averaged internal clock. We take the tendency for faster-than-logarithmic growth of Se(t) together with the smooth dependency on W of all our observables within the entire simulation window as support for the crossover scenario, discouraging an MBL transition within the traditional parametric-window of computational studies.