Spatial source-area analysis of three-dimensional moisture fields from lidar, eddy covariance, and a footprint model

Abstract The Los Alamos National Laboratory scanning Raman lidar was used to measure the three-dimensional moisture field over a salt cedar canopy. A critical question concerning these measurements is; what are the spatial properties of the source region that contributes to the observed three-dimensional moisture field? Traditional methods used to address footprint properties rely on point sensor time-series data and the assumption of Taylor’s hypothesis to transform temporal data into the spatial domain. In this paper, the analysis of horizontal source-area size is addressed from direct lidar-based spatial analysis of the moisture field, eddy covariance co-spectra, and a dedicated footprint model. The results of these analysis techniques converged on the microscale average source region of between 25 and 75 m under ideal conditions. This work supports the concept that the scanning lidar can be used to map small scale boundary layer processes, including riparian zone moisture fields and fluxes.

[1]  D. Baldocchi Flux Footprints Within and Over Forest Canopies , 1997 .

[2]  J. C. Kaimal,et al.  Atmospheric boundary layer flows , 1994 .

[3]  G. W. Thurtell,et al.  A Lagrangian Solution To The Relationship Between A Distributed Source And Concentration Profile , 2000 .

[4]  Wilfried Brutsaert,et al.  Evaporation into the atmosphere : theory, history, and applications , 1982 .

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

[6]  William P. Kustas,et al.  Spatial mapping of evapotranspiration and energy balance components over riparian vegetation using airborne remote sensing , 2001 .

[7]  Analysis of flux maps versus surface characteristics from Twin Otter grid flights in BOREAS 1994 , 1997 .

[8]  D. B. Holtkamp,et al.  Spatial variability of water vapor turbulent transfer within the boundary layer , 1992 .

[9]  Cheng-I Hsieh,et al.  Spatial Variability of Turbulent Fluxes in the Roughness Sublayer of an Even-Aged Pine Forest , 1999 .

[10]  J. Laubach,et al.  Power Spectra and Cospectra for Wind and Scalars in a Disturbed Surface Layer at the Base of an Advective Inversion , 2000, Boundary-Layer Meteorology.

[11]  B. Lamb,et al.  Observations and large-eddy simulation modeling of footprints in the lower convective boundary layer , 1997 .

[12]  T. W. Horst,et al.  Experimental evaluation of analytical and Lagrangian surface-layer flux footprint models , 1996 .

[13]  C. R. Quick,et al.  Development of a scanning, solar-blind, water Raman lidar. , 1994, Applied optics.

[14]  Franz Durst,et al.  Turbulent Shear Flows I , 1979 .

[15]  J. Monteith,et al.  Principles of Environmental Physics , 2014 .

[16]  William E. Eichinger,et al.  High-resolution properties of the Equatorial Pacific marine atmospheric boundary layer from lidar and radiosonde observations , 1996 .

[17]  L. C. Chen,et al.  Estimation of spatially distributed latent heat flux over complex terrain from a Raman lidar , 2000 .

[18]  Steven R. Hanna,et al.  Lagrangian and Eulerian Time-Scale Relations in the Daytime Boundary Layer , 1981 .

[19]  Monique Y. Leclerc,et al.  Footprint prediction of scalar fluxes from analytical solutions of the diffusion equation , 1990 .

[20]  R. Stull An Introduction to Boundary Layer Meteorology , 1988 .