Examination of the Bouchet Morton Complementary Relationship Using a Mesoscale Climate Model and Observations under a Progressive Irrigation Scenario

The complementary relationship between actual and potential evaporation over southeastern Turkey was examined using a mesoscale climate model and field data. Model simulations of both actual and potential evaporation produce realistic temporal patterns in comparison to those estimated from field data; as evaporation from the surface increases with increasing irrigation, potential evaporation decreases. This is in accordance with the Bouchet–Morton complementary relationship and suggests that actual evapotranspiration can be readily computed from routine meteorological observations. The driving mechanisms behind irrigation-related changes in actual and potential evaporation include reduced wind velocities, increased atmospheric stability, and depressed humidity deficits. The relative role of each in preserving the complementary relation is assessed by fitting a potential evaporation model to pan evaporation data. The importance of reduced wind velocity in maintaining complementarity was unexpected, and thus examined further using a set of perturbation simulation experiments with changing roughness parameters (reflecting growing cotton crops), changing moisture conditions (reflecting irrigation), and both. Three potential causes of wind velocity reduction associated with irrigation may be increased surface roughness, decreased thermal convection that influences momentum transfer, and the development of anomalous high pressure that counteracts the background wind field. All three are evident in the mesoscale model results, but the primary cause is the pressure-induced local wind system. The apparent necessity of capturing mesoscale dynamical feedbacks in maintaining complementarity between potential and actual evaporation suggests that a theory more complicated than current descriptions (which are based on feedbacks between actual evaporation and temperature and/or humidity gradients) is required to explain the complementary relationship.

[1]  H. L. Penman Natural evaporation from open water, bare soil and grass , 1948, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[2]  A S Monin,et al.  BASIC LAWS OF TURBULENT MIXING IN THE GROUND LAYER OF ATMOSPHERE , 1954 .

[3]  F. I. Morton Potential Evaporation and River Basin Evaporation , 1965 .

[4]  C. Priestley,et al.  On the Assessment of Surface Heat Flux and Evaporation Using Large-Scale Parameters , 1972 .

[5]  Marvin E. Jensen,et al.  Changes in Climate and Estimated Evaporation Across a Large Irrigated Area in Idaho , 1975 .

[6]  Wilfried Brutsaert,et al.  An advection-aridity approach to estimate actual regional evapotranspiration. , 1979 .

[7]  C. Willmott Some Comments on the Evaluation of Model Performance , 1982 .

[8]  W. Brutsaert Evaporation into the atmosphere , 1982 .

[9]  M. Ek,et al.  The Influence of Atmospheric Stability on Potential Evaporation , 1984 .

[10]  P. Alpert,et al.  Wind Variability--An Indicator for a Mesoclimatic Change in Israel. , 1986 .

[11]  S. P. S. Arya,et al.  Introduction to micrometeorology , 1988 .

[12]  T. W. Spriggs,et al.  An evaluation of the Priestley and Taylor equation and the complementary relationship using results from a mixed-layer model of the convective boundary layer , 1989 .

[13]  R. Pielke,et al.  The Impact of Crop Areas in Northeast Colorado on Midsummer Mesoscale Thermal Circulations , 1989 .

[14]  Marc B. Parlange,et al.  Estimation of the diurnal variation of potential evaporation from a wet bare soil surface , 1992 .

[15]  R. Arritt,et al.  Nonclassical mesoscale circulations caused by surface sensible heat-flux gradients , 1992 .

[16]  J. Garratt The Atmospheric Boundary Layer , 1992 .

[17]  Fei Chen,et al.  Development and analysis of prognostic equations for mesoscale kinetic energy and mesoscale (subgrid scale) fluxes for large-scale atmospheric models , 1993 .

[18]  M. Kanamitsu,et al.  The NMC Nested Regional Spectral Model , 1994 .

[19]  Fei Chen,et al.  The impact of land-surface wetness heterogeneity on mesoscale heat fluxes , 1994 .

[20]  M. S. Moran,et al.  Sensible heat flux - Radiometric surface temperature relationship for eight semiarid areas , 1994 .

[21]  J. Doran,et al.  Boundary layer characteristics over areas of inhomogeneous surface fluxes , 1995 .

[22]  H. Pan,et al.  Nonlocal Boundary Layer Vertical Diffusion in a Medium-Range Forecast Model , 1996 .

[23]  Y. Xue,et al.  Modeling of land surface evaporation by four schemes and comparison with FIFE observations , 1996 .

[24]  R. Reynolds,et al.  The NCEP/NCAR 40-Year Reanalysis Project , 1996, Renewable Energy.

[25]  J. Lhomme,et al.  A THEORETICAL BASIS FOR THE PRIESTLEY-TAYLOR COEFFICIENT , 1997 .

[26]  Song-You Hong,et al.  The NCEP Regional Spectral Model: An Update , 1997 .

[27]  Dara Entekhabi,et al.  Examination of two methods for estimating regional evaporation using a coupled mixed layer and land surface model , 1997 .

[28]  Influence of components of the advection-aridity approach on evapotranspiration estimation , 1997 .

[29]  Koen De Ridder,et al.  Land Surface-Induced Regional Climate Change in Southern Israel , 1998 .

[30]  Wilfried Brutsaert,et al.  Aspects of bulk atmospheric boundary layer similarity under free‐convective conditions , 1999 .

[31]  B. Anderson,et al.  Regional simulation of the low‐level monsoon winds over the Gulf of California and southwestern United States , 2000 .

[32]  Michael R. Raupach,et al.  Equilibrium Evaporation and the Convective Boundary Layer , 2000, Boundary-Layer Meteorology.

[33]  J. Szilágyi On Bouchet's complementary hypothesis , 2001 .

[34]  T. Brown,et al.  The complementary relationship in estimation of regional evapotranspiration: The complementary relationship areal evapotranspiration and advection‐aridity models , 2001 .

[35]  Complementary relationship with a convective boundary layer model to estimate regional evaporation , 2001 .

[36]  B. Anderson,et al.  The Summertime Atmospheric Hydrologic Cycle over the Southwestern United States , 2004 .

[37]  Mutlu Ozdogan,et al.  Irrigation‐induced changes in potential evapotranspiration in southeastern Turkey: Test and application of Bouchet's complementary hypothesis , 2004 .

[38]  Thomas C. Brown,et al.  Trends in pan evaporation and actual evapotranspiration across the conterminous U.S.: Paradoxical or complementary? , 2004 .

[39]  Curtis E. Woodcock,et al.  Changes in Summer Irrigated Crop Area and Water Use in Southeastern Turkey from 1993 to 2002: Implications for Current and Future Water Resources , 2006 .