7Infiltration is dominantly gravity driven. Thus, the 8 viscous-flow approach to infiltration and drainage is 9 based on laminar film flow. Its hydro-mechanical base is 10 the equilibrium between the viscous and the gravity 11force. This leads to a constant flow velocity during a period lasting 3/2 times the duration of a constant 12 input rate, qS. The key parameters of the approach are the film thickness F and the specific contact 13 area L of the film per unit soil volume. Calibration of the approach requires at some depth any pair of 14 the three time functions volume flux density, mobile water content, and velocity of the wetting front. 15Sprinkler irrigation produces in-situ time series of volumetric water contents, θ(z,t), as determined 16 with TDR-probes. The wetting front velocity v and the time series of the mobile water content, w(z,t) 17 are deduced from θ(z,t). In-vitro steady flow in a core of saturated soil provides volume flux density, 18 q(z,t), and flow velocity, v, as determined from heat front velocity. The viscous-flow approach is 19 introduced in details, and the F-and L-parameters of the in-situ and the in-vitro experiments are 20 compared. The macropore-flow restriction states that, for a particular permeable medium, the specific 21 contact area L be independent from qs i.e., dL/dqS = 0. If true, than the relationship of qS v 3/2 could 22 scale a wide range of input rates 0 < qS < Ksat into a particular permeable medium, and kinematic-wave 23 theory would become a versatile tool to deal with non-equilibrium flow. The viscous-flow approach is 24 based on hydro-mechanical principles similar to Darcy's (1856) law, but currently it is not suited to 25 deduce flow properties from specified individual spatial structures of permeable media. 26