“…At all times, the saturation presents a discontinuity in x = 0.5, due to the fact that, since both phases flow at this location, the gas and the liquid pressures must remain continuous. Therefore, the saturation must respect the equation P (1) c (S (1) l (0.5, t)) = P (2) c (S (2) l (0.5, t)), where upper indices (1) and (2) denote the values and functions respectively available in regions M1 and M2, at all times t > 0, which leads to different left and right limits of the saturation in x = 0.5. At large times, the liquid pressure becomes constant, which is expected since the water phase is mobile in the whole domain, and therefore the liquid saturation, resulting from the capillary curves and the difference between the gas and the liquid pressures, becomes constant in M1 and M2.…”