Connections between groundwater flow and transpiration partitioning

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Connections between groundwater flow and transpiration partitioning by Reed M. Maxwell, and Laura E. Condon Science Volume 353(6297):377-380 July 22, 2016 Published by AAAS

Fig. 1 Simulation results display great spatial complexity. Simulation results display great spatial complexity. Plots of transient (water year 1985) annually averaged water table (WT) depth (A) and LH flux (B) demonstrate the great detail we see in this simulation. Water table varies with climatic region; it is generally deeper west of the aridity divide and shallower in the east. Likewise, LH flux is also greater in less water-limited regions but exhibits larger values in river valleys, where the water table depths are locally shallow under what might otherwise be water-limited conditions. Reed M. Maxwell, and Laura E. Condon Science 2016;353:377-380 Published by AAAS

Fig. 2 Simulated annually averaged histograms of evapotranspiration partitioning compare favorably to observations and are related to water table depth. Simulated annually averaged histograms of evapotranspiration partitioning compare favorably to observations and are related to water table depth. Simulated T/ET ratios (A and B) plotted by land cover type agree with stand-scale estimates and observations (14) and are bracketed by global isotopic estimates, isotopic 1 (4) and isotopic 2 (20, 21), shown here as box plots spanning the ± mean 1 SD. Scatterplots of water table versus LH flux (C), bare soil evaporation (D), and T (E) suggest that groundwater’s role in moderating these fluxes (7–9, 27) extends across our continental-scale domain. When plotted as a function of water table depth, the T/E ratio (F) peaks at the middle of the groundwater critical depth range, suggesting that T may be as much as 35 times greater than E because of lateral groundwater flow. Reed M. Maxwell, and Laura E. Condon Science 2016;353:377-380 Published by AAAS

Fig. 3 The relationship between groundwater depth and land-energy fluxes for an idealized hillslope. The relationship between groundwater depth and land-energy fluxes for an idealized hillslope. On the left, groundwater (GW) is shallow and neither T or E is water-limited, because of lateral groundwater convergence, which stabilizes soil moisture. On the far right, groundwater is deep and disconnected from the land surface, resulting in lower T and E that are limited by precipitation. In the two center regions, T or E varies with groundwater depth, but E disconnects at shallower depths than T. As a result of these behaviors, T/E partitioning is sensitive to water table depth across both center regions. The peak in T/E reflects the differential in response to water table changes in E as compared to T. The roots as drawn here are not to scale and do not reflect potential changes in density due to water table depth, nor does this figure reflect the presence of subsurface heterogeneity. Reed M. Maxwell, and Laura E. Condon Science 2016;353:377-380 Published by AAAS