“…As asserted by Dooge (1986), "within the physical sciences and the Earth sciences there is and can be no universal model for water movement." Despite numerous attempts at integrating local models across soils (e.g., Kim et al, 1997), hillslopes , and watersheds (e.g., Reggiani et al, 1998Reggiani et al, , 1999Reggiani et al, , 2000Reggiani et al, , 2001, universal laws in hydrology and the required closure relations remain elusive because the physics are likely scale-dependent (e.g., Bierkens, 1996) and the data required to test these hypotheses are either not readily available or not easily synthesized, or, even worse, would never be observable (Beven, 2006). Further, computational advances have enabled so-called "hyperresolution" or, using an alternative term that is not necessarily equivalent, "hillslope-resolving" modeling (e.g., Chaney et al, 2016;Wood et al, 2011); but as noted in the discussion between Beven and Cloke (2012) and Wood et al (2012), and later discussed in Beven et al (2015), the ability to provide meaningful information from hillslope-resolving models is limited both by a lack of tested parameterizations on a given model scale as well as by lack of data for model evaluation (e.g., Melsen et al, 2016a).…”