The complementary principle (Bouchet, 1963) results a relationship between the actual evaporation (E) from a landscape under natural condition, the apparent potential evaporation ( 𝐴𝐴 𝐴𝐴pa ) of a small saturated surface inside the natural landscape and the potential evaporation ( 𝐴𝐴 𝐴𝐴po ) that occurs from the landscape when it is well watered (Brutsaert, 2015). The complementary relationship (CR) arises from the land-atmosphere coupling via landscape evaporation and atmospheric evaporative demand, and offers the advantages of estimating the actual evaporation using routinely measured meteorological variables only (Brutsaert, 2005;. The atmospheric evaporative demand 𝐴𝐴 𝐴𝐴pa can be measured by means of standard evaporation pans or calculated by Penman ( 1948)'s open water evaporation, while 𝐴𝐴 𝐴𝐴po is thought to be limited by the available energy (Brutsaert & Stricker, 1979;Morton, 1983). The CR was originally referred to that E and 𝐴𝐴 𝐴𝐴pa deviate from 𝐴𝐴 𝐴𝐴po with equal but opposite changes along with the drying of the landscape (Bouchet, 1963), and is supported by the opposite changes in the actual and pan evaporations with the progressive expansion of irrigated land as a "natural" experiment (Han et al., 2014;Ozdogan & Salvucci, 2004;Roderick et al., 2009). The original symmetric CR was extended to an asymmetric linear relationship representing opposite changes of E and 𝐴𝐴 𝐴𝐴pa (Brutsaert & Parlange, 1998), and has evolved to generalized nonlinear functions (