Abstract:Non‐closure of the surface energy balance is a frequently observed phenomenon of hydrometeorological field measurements, when using the eddy‐covariance method, which can be ascribed to an underestimation of the turbulent fluxes. Several approaches have been proposed in order to adjust the measured fluxes for this apparent systematic error. However, there are uncertainties about partitioning of the energy balance residual between the sensible and latent heat flux and whether such a correction should be applied … Show more
“…For all FLUXNET site data, an overall mean energy imbalance of about 20% was observed (Wilson et al, ), signifying that in contrast to the theoretical basis of energy conservation implicit in Equation , the nonturbulent fluxes exceed the turbulent fluxes. This energy balance gap is often associated with energy transport of large scale eddies, which is not quantified accurately with the EC method and a 30‐min averaging interval (Foken, ; Mauder et al, ). Foken () described difficulties of model calibration associated with the energy balance gap.…”
Section: Methodsmentioning
confidence: 99%
“…Ingwersen, Imukova, Högy, & Streck, ); however, we decided to correct Q E by partitioning the energy balance residual (Δ Q ) according to the Bowen ratio β (Twine et al, ; Equation ) in order to adjust ET a . Using this closure procedure, we assume the scalar similarity of gas and heat exchange not only for small scale but also for large‐scale eddies (Foken, ; Mauder et al, ). The median diurnal course of β was determined from the flux data from July and August and used for the correction for every time of the day as it allows to represent the variation of β through the course of the day and it is robust against measurement uncertainties of individual flux measurements.…”
Section: Methodsmentioning
confidence: 99%
“…The parameter estimation results for the crop coefficient, K c* (−), and coefficients of determination (R 2 ) as an indication for the goodness are given scalar similarity(Ruppert, Thomas, & Foken, 2006). Nonetheless,Mauder et al (2018) could achieve a better agreement of ET rates from EC experiments with lysimeter ET rates by applying Bowen ratio based energy balance gap correction. Without a correction, the uncorrected K c* estimates had a range of 0.68-0.76, which is implausibly low and its interannual variability implausibly large.…”
In the soil–plant–atmosphere continuum, fluxes of water, energy, and carbon determine the water and carbon balance of peat bogs. We used eddy covariance (EC) measurements to study surface atmosphere exchange and its drivers above an ombrotrophic peat bog (Odersprungmoor) in the Harz Mountains, Germany, with nonideal measurement conditions during the growing season in 2013. For montane peatlands, only very few EC flux measurements exist due to site constraints, for example, surface slope, limited fetch, and frequent dew formation on open path sensors. The measured data were carefully filtered resulting in valid and representative fluxes for the bog. The evapotranspiration (ET) was further characterized by determining the adjusted crop coefficient (Kc*) for July and August and comparing it with Kc* values from 7 years of the FLUXNET site Mer Bleue bog, Ontario, Canada. While soil moisture was taken into consideration, the adjustment was nevertheless necessary as plant health and nutrient supply were not evaluated as required by FAO guidelines. Actual ET at OM was well described by the Kc* model (Kc* = 0.85, R2 = 0.85). The primary control on ET was available energy and atmospheric conditions and, marginally, the soil moisture conditions. This Kc* value is comparable to the calculated Kc* values for MB, which ranged between 0.82 and 0.86 (R2 between 0.84 and 0.97). Since these Kc* ranges are narrow for the different sites and years, we hypothesize that these values are good estimates for the true crop coefficients of Sphagnum‐dominated peat bogs.
“…For all FLUXNET site data, an overall mean energy imbalance of about 20% was observed (Wilson et al, ), signifying that in contrast to the theoretical basis of energy conservation implicit in Equation , the nonturbulent fluxes exceed the turbulent fluxes. This energy balance gap is often associated with energy transport of large scale eddies, which is not quantified accurately with the EC method and a 30‐min averaging interval (Foken, ; Mauder et al, ). Foken () described difficulties of model calibration associated with the energy balance gap.…”
Section: Methodsmentioning
confidence: 99%
“…Ingwersen, Imukova, Högy, & Streck, ); however, we decided to correct Q E by partitioning the energy balance residual (Δ Q ) according to the Bowen ratio β (Twine et al, ; Equation ) in order to adjust ET a . Using this closure procedure, we assume the scalar similarity of gas and heat exchange not only for small scale but also for large‐scale eddies (Foken, ; Mauder et al, ). The median diurnal course of β was determined from the flux data from July and August and used for the correction for every time of the day as it allows to represent the variation of β through the course of the day and it is robust against measurement uncertainties of individual flux measurements.…”
Section: Methodsmentioning
confidence: 99%
“…The parameter estimation results for the crop coefficient, K c* (−), and coefficients of determination (R 2 ) as an indication for the goodness are given scalar similarity(Ruppert, Thomas, & Foken, 2006). Nonetheless,Mauder et al (2018) could achieve a better agreement of ET rates from EC experiments with lysimeter ET rates by applying Bowen ratio based energy balance gap correction. Without a correction, the uncorrected K c* estimates had a range of 0.68-0.76, which is implausibly low and its interannual variability implausibly large.…”
In the soil–plant–atmosphere continuum, fluxes of water, energy, and carbon determine the water and carbon balance of peat bogs. We used eddy covariance (EC) measurements to study surface atmosphere exchange and its drivers above an ombrotrophic peat bog (Odersprungmoor) in the Harz Mountains, Germany, with nonideal measurement conditions during the growing season in 2013. For montane peatlands, only very few EC flux measurements exist due to site constraints, for example, surface slope, limited fetch, and frequent dew formation on open path sensors. The measured data were carefully filtered resulting in valid and representative fluxes for the bog. The evapotranspiration (ET) was further characterized by determining the adjusted crop coefficient (Kc*) for July and August and comparing it with Kc* values from 7 years of the FLUXNET site Mer Bleue bog, Ontario, Canada. While soil moisture was taken into consideration, the adjustment was nevertheless necessary as plant health and nutrient supply were not evaluated as required by FAO guidelines. Actual ET at OM was well described by the Kc* model (Kc* = 0.85, R2 = 0.85). The primary control on ET was available energy and atmospheric conditions and, marginally, the soil moisture conditions. This Kc* value is comparable to the calculated Kc* values for MB, which ranged between 0.82 and 0.86 (R2 between 0.84 and 0.97). Since these Kc* ranges are narrow for the different sites and years, we hypothesize that these values are good estimates for the true crop coefficients of Sphagnum‐dominated peat bogs.
“…Comprehensive long‐term integrated observations in different compartments (atmosphere, hydrosphere, biosphere) of the terrestrial system are used to set up, further develop, and apply various process models for site‐ and regional‐scale or catchment‐scale simulations. The evaluation of the energy balance closure problem for evapotranspiration estimates (Mauder et al, 2018) and the methodology development to use commercial microwave links for precipitation quantification and improved discharge modeling (Smiatek et al, 2017) are prominent examples. TERENO Pre‐Alpine observations have been used in conjunction with physically based process models to examine the impacts of land cover–management and climate change on ecosystem‐atmosphere cycling of energy (e.g., large‐eddy simulation model PALM; Maronga et al [2015]), water (e.g., WaSiM and GEOtop; Kunstmann et al, 2006), as well as C and N (e.g., LandscapeDNDC; Haas et al [2013]).…”
Section: Lessons Learned and Future Perspectivesmentioning
Global change has triggered several transformations, such as alterations in climate, land productivity, water resources, and atmospheric chemistry, with far reaching impacts on ecosystem functions and services. Finding solutions to climate and land cover change-driven impacts on our terrestrial environment is one of the most important scientific challenges of the 21st century, with farreaching interlinkages to the socio-economy. The setup of the German Terrestrial Environmental Observatories (TERENO) Pre-Alpine Observatory was motivated by the fact that mountain areas, such as the pre-alpine region in southern Germany, have been exposed to more intense warming compared with the global average trend and to higher frequencies of extreme hydrological events, such as droughts and intense rainfall. Scientific research questions in the TERENO Pre-Alpine Observatory focus on improved process understanding and closing of combined energy, water, C, and N cycles at site to regional scales. The main long-term objectives of the TERENO Pre-Alpine Observatory include the characterization and quantification of climate change and land cover-management effects on terrestrial hydrology and biogeochemical processes at site and regional scales by joint measuring and modeling approaches. Here we present a detailed climatic and biogeophysical characterization of the TERENO Pre-Alpine Observatory and a summary of novel scientific findings from observations and projects. Finally, we reflect on future directions of climate impact research in this particularly vulnerable region of Germany.
“…Studies have shown that the surface temperature, outgoing longwave radiation, cooling rates, and frozen surface extent are sensitive to far-infrared surface emissivity [8,9]. z 0m and z 0h are defined as the height at which the wind speed becomes zero and at which the extrapolated air temperature is identical to the surface temperature over a homogeneous surface under neutral and thermally stratified conditions [10][11][12], respectively, and they are very important parameters for estimating the momentum, heat, and mass exchange between the surface and atmosphere [13][14][15][16][17][18][19]. They are generally estimated directly using the eddy covariance method and satellite data inversion technique [20,21].…”
An observational data set of the year 2010 at a site in the northern marginal zone of the Taklimakan Desert (TD) was used to analyse the key surface parameters in land-atmospheric interactions in the desert climate of northwest China. We found that the surface albedo (α) and emissivity (ε) were 0.27 and 0.91, respectively, which were consistent with the values obtained based on observations in the hinterland of the TD as well as being similar to the dry parts of the Great Basin desert in North America, where they were comparable to the α and ε values retrieved from remote sensing products. Peak frequency value of z 0m was 5.858 × 10 −3 m, which was similar to the Mojave Desert, Peruvian desert, Sonoran Desert, HEIFE (Heihe region) Desert, and Badain Jaran Desert. The peak frequency value of z 0h was 1.965 × 10 −4 m, which was different from those obtained in the hinterland of the TD. The average annual value of excess resistance to heat transfer (kB −1 ) was 2.5, which was different from those obtained in the HEIFE Gobi and desert, but they were similar to those determined for the Qinghai-Tibetan Plateau and HAPEX-Sahel. Both z 0m and z 0h varied less diurnally but notably seasonally, and kB −1 exhibited weak diurnal and seasonal variations. We also found that z 0m was strongly influenced by the local wind direction. There were many undulating sand dunes in the prevailing wind and opposite to the prevailing wind, which were consistent with the directions of the peak z 0m value. The mean values calculated over 24 h for C d and C h were 6.34 × 10 −3 and 5.96 × 10 −3 , respectively, which were larger than in the Gobi area, hinterland of the TD and semiarid areas, but similar to HEIFE desert. Under the normal prevailing (NNE-ESE) wind, the mean bulk transfer coefficient C d and C h were of the same order of magnitude as expected based on similarity theory. Using the data obtained under different wind directions, we determined the relationships between C d , C h , the wind speed U, and stability parameter z/L, and the results were different. C d and C h decreased rapidly as the wind speed dropped below 3.0 m s −1 and their minimum values reached around 1-2 m s −1 . It should also be noted that the ε values estimated using the sensible heat flux (H) were better compared with those produced using other estimation methods.
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