Testing of a higher-order closure model for modeling airflow within and above plant canopies

A higher-order closure model was developed to simulate airflow within and above vegetative environments. The model consists of equations for the mean wind, turbulent kinetic energy (TKE) components, tangential stress and simplified equations for the third-order transport terms that appear in the second-order equations. The model in general successfully simulated wind speed profiles within and above maize, been, soybeen, wheat, orange and spruce canopies. Profiles of % MathType!MTEF!2!1!+-% feaafeart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaa0aaaeaace% WG1bGbauaadaahaaWcbeqaaiaaikdaaaaaaaaa!37EC!\[\overline {u'^2 } \] and % MathType!MTEF!2!1!+-% feaafeart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaa0aaaeaace% WG3bGbauaadaahaaWcbeqaaiaaikdaaaaaaaaa!37EE!\[\overline {w'^2 } \] for the maize canopy were overestimated near the top of the canopy where both shear and wake production of TKE are high. These errors are believed to be caused by incorrect parameterizations for either the dissipation rate of TKE and/or the pressure-velocity correlations in the budget equations for the second moments.

[1]  A. Thom Momentum absorption by vegetation , 1971 .

[2]  J. Landsberg,et al.  WIND PROFILES IN PLANT CANOPIES: STUDIES ON AN ANALYTICAL MODEL , 1971 .

[3]  G. Stanhill,et al.  The climate of an orange orchard: Physical characteristics and microclimate relationships , 1972 .

[4]  Brian Launder,et al.  A Reynolds stress model of turbulence and its application to thin shear flows , 1972, Journal of Fluid Mechanics.

[5]  George L. Mellor,et al.  Analytic Prediction of the Properties of Stratified Planetary Surface Layers , 1973 .

[6]  J. Lumley Pressure‐strain correlation , 1975 .

[7]  H. Tennekes,et al.  A Self-Contained Model for the Pressure Terms in the Turbulent Stress Equations of the Neutral Atmospheric Boundary Layer , 1975 .

[8]  Otto Zeman,et al.  Modeling Buoyancy Driven Mixed Layers , 1976 .

[9]  R. Shaw Secondary Wind Speed Maxima Inside Plant Canopies , 1977 .

[10]  N. Wilson,et al.  A Higher Order Closure Model for Canopy Flow , 1977 .

[11]  T. Maitani Vertical transport of turbulent kinetic energy in the surface layer over a paddy field , 1977 .

[12]  Turbulence in waving wheat , 1979 .

[13]  Y. Ogura,et al.  Modeling the Evolution of the Convective Planetary Boundary Layer , 1980 .

[14]  A. Thom,et al.  Turbulence in and above Plant Canopies , 1981 .

[15]  G. W. Thurtell,et al.  Numerical simulation of particle trajectories in inhomogeneous turbulence, III: Comparison of predictions with experimental data for the atmospheric surface layer , 1981 .

[16]  Third- and fourth-order mixed moments of turbulent velocity and temperature fluctuations in the atmospheric surface layer , 1982 .

[17]  M. Raupach,et al.  Averaging procedures for flow within vegetation canopies , 1982 .

[18]  Mass and Energy Exchanges of Soybeans: Microclimate-Plant Architectural Interactions , 1982 .

[19]  J. Andre,et al.  Pressure effects on triple correlations in turbulent convective flows , 1982 .

[20]  G. W. Thurtell,et al.  Statistics of atmospheric turbulence within and above a corn canopy , 1982 .

[21]  R. Shaw,et al.  Structure of the Reynolds Stress in a Canopy Layer , 1983 .

[22]  E. F. Bradley,et al.  Flux-Gradient Relationships in a Forest Canopy , 1985 .

[23]  M. Raupach,et al.  Experiments on scalar dispersion within a model plant canopy part I: The turbulence structure , 1986 .