Wolf Creek Research Basin: Hydrology, Ecology, Environment Partitioning of Energy During the Snow-free Season at the Wolf Creek Research Basin Raoul J. Granger National Water Research Institute, National Hydrology Research Centre, Environment Canada, Saskatoon, Saskatchewan, S7N 3H5 Abstract The results of four years of observation of the partitioning of energy at three sites in the Wolf Creek Research Basin are presented. The sites are representative of the major land use classes in the basin, boreal forest, high bush tundra and alpine tundra, and range in elevation from 750 to 1600 m. The instrumentation deployed allows for the determination of the complete energy and water balances at these sites. The data from these sites are also used in the development of parameterizations for the modelling of evapotranspiration and the application of remote sensing to the estimate of regional evapotranspiration. The energy balances are derived and presented for the three Wolf Creek sites. Net radiation and soil heat fluxes are measured directly, and the turbulent fluxes are derived from measurements of temperature, humidity and wind speeds observed at the sites. Results from the 1994-1997 snow-free periods are presented. Seasonal trends, as well as the differences between the sites (land cover and elevation), are demonstrated. Introduction Wolf Creek basin, near Whitehorse, Yukon Territory, has been the site of intense investigations of the processes governing the energy and water balance components in a high latitude environment. It has been designated as one of the major study sites for the Canadian GEWEX programme; which has amongst its objectives the achievement of an improved understanding of cold region, high latitude hydrological and meteorological processes and the role that they play in the global climate system. In the understanding of climatic change and the assessment of its effects, the correct evaluation of the partitioning of energy at the surface, and of the role evapotranspiration will play in a modified hydrological cycle, becomes crucial in regions such as the Canadian Prairies and the North. Most current operational evapotranspiration models ignore the effects of changes in soil heat storage. In regions where the seasonal soil heat storage effects are important, these models must be modified to take these effects into account. 33 Granger - Evaporation Wolf Creek Site Description and Instrumentation The Wolf Creek basin, located 15 kilometres south of Whitehorse, Yukon Territory, occupies a 195 km2 area which forms part of the headwater region for the Yukon River. The basin elevation ranges from 750 to 2250 m. The area is within the discontinuous/scattered permafrost zone with sporadic permafrost at higher elevations and on north-facing slopes. The watershed has three broad vegetation cover types of about equal proportions; these are alpine tundra, shrub taiga and boreal forest consisting of mixed spruce, pine and poplar. The three broad vegetation cover types present in the basin are representative of the major vegetation cover types found from the boreal forest of Western Canada to the high arctic tundra. The basin is thus a convenient, relatively compact outdoor laboratory offering three of the major vegetation types found in the Mackenzie Basin. As well, the presence of permafrost on some higher and north-facing slopes makes this basin an appropriate site for undertaking comparative studies of the hydrological effects of permafrost. Micrometeorological instrument sites were established at representative locations within each of the three vegetation zones in the basin. The alpine tundra site, at an elevation of 1615 m, is situated on a wind-swept, high alpine tundra plateau which defines part of the drainage divide along the northern edge of the basin. A reasonably-level fetch extends for approximately 100 m in all directions; to the north, south and west the terrain drops towards the respective valleys, while to the east the terrain rises slightly to a rounded hilltop. Vegetation is sparse and consists of mosses and lichens with occasional patches of scrub willow and birch no more than 20 cm tall. The plateau is also strewn with boulders. The shrub taiga site, at an elevation of 1250 m, is located near the bottom of a glacial valley in the upper reaches of the basin. There is a slightly sloping fetch NE and SW for several km; to the SE the valley slopes up and to the NW the valley drops somewhat before rising to the next ridge. The vegetation consists mainly of tall willows and alders, ranging from 1 to 2 m in height, with very scattered spruce. The forest site (elevation of 750 m) is in a mature white spruce stand on a flat valley bottom; the vegetation height ranges from 15 to 18 m. The site is located near the basin outlet. Each of these sites contained the core instrumentation to monitor the vertical water and energy balance; the following parameters were recorded: net all-wave radiation, incoming and reflected short-wave radiation, air temperature*, relative humidity*, wind speed* and direction, infrared canopy surface temperature, soil heat flux, soil temperature*, rainfall, snowfall and depth of snow on the ground. Barometric pressure was also observed at the Alpine station. (* Denotes those parameters measured at two or more levels.) 34 Wolf Creek Research Basin: Hydrology, Ecology, Environment Data were automatically-recorded every half hour; each recording represents the average of the individual readings sampled at 15 second intervals. For the study period, the data stream is continuous and uninterrupted. For the purpose of obtaining the daily energy balance terms, the daily average values were computed based on the 24-hr period from midnight to midnight Pacific Daylight Time. Energy Balance The energy balance of a surface can be expressed by the equation, (1) where Rn is the net all-wave radiation to the surface, Qg is the heat flux into the soil surface, LE and H are the turbulent latent and sensible heat fluxes above the surface. In Eq. 1, the net radiation term, Rn, was measured directly. Because daily time periods were used, the changes in energy stored in the soil layer above the soil heat flux sensors were ignored, and the soil heat flux sensor readings were used directly to represent the soil heat term, Qg. The latent heat term, LE, was estimated using an evapotranspiration model (described below), and the sensible heat term, H, was determined as the residual in the balance equation (1). Calculating the sensible heat as the residual in Eq. 1 means that it includes (for the surfaces with significant vegetation) the change in heat storage within the vegetation canopy; however, since daily totals are considered, this component is small compared to the turbulent flux itself and is generally ignored. The components of the energy balance are expressed in equivalent millimetres of evaporation by dividing each term by the latent heat of vaporization, L. The energy balance equation presented in the form of Eq. 1 actually represents the partitioning of the incoming radiation into the three major fluxes, such that a net radiation flux directed toward the surface is given a positive sign, while the soil heat, sensible and latent heat terms are considered positive if directed away from the surface. Evapotranspiration Model The daily evapotranspiration, E, was estimated using an algorithm developed by Granger and Gray (1989) and Granger (1991). The method is based on an extension of the Penman (1948) equation to the non-saturated case. The method is also consistent with the feedback approach described by Bouchet (1963). The 35 Granger - Evaporation general equation for evaporation from non-saturated surfaces, as derived by Granger and Gray (1989) is given as (2) where, ∆ is the slope of the saturation vapour pressure vs temperature curve; G is a dimensionless relative evaporation parameter; γ is the psychrometric constant and Ea is the drying power of the air, as defined by Penman (1948). The fluxes, Rn, Qg, and Ea are in units of mm/d equivalent evaporation. The drying power, Ea, can be obtained using a Dalton-type formulation: (3) where, ea is the actual vapour pressure of the air (expressed in kPa), e* is the saturated vapour pressure of the air at the actual air temperature, and ƒ(u), the vapour transfer coefficient, is a function of wind speed when applied to a daily period: (4) where the average wind speed, u, is given in m/s. The constants a and b are related to the surface roughness using the following expressions derived in the southern boreal forest (Pomeroy et al., 1997): (5a) (5b) in which the roughness length, Z0 , is given in cm. The relative evaporation, G, is related to a dimensionless relative drying power, D. D is defined as: (6) and (7) Eq. 7 was derived using data obtained over a variety of surfaces including bare soil, grass, growing wheat, and aspen forest, and it appears to be applicable to all these surfaces; the differences in surface characteristics being accounted for in 36 Wolf Creek Research Basin: Hydrology, Ecology, Environment the terms Ea (surface roughness) and Rn (albedo). Eq. 7 is limited to those situations for which the value of the relative drying power, D, falls between zero and unity, that is, only for those conditions in which the period available energy (Rn-Qg) is positive. This, however, is a limitation which applies to all evapotranspiration models which utilize a form of the Penman equation. When working with daily time periods, especially during the growing season, the available energy is almost always positive. For those periods when the available energy is negative, an alternative approach must be used; a regression approach, such as the Priestley-Taylor (1972) approach can be used if suitable coefficients have been derived for the surface conditions encountered. Based on comparisons with eddy correlation measurements obtained over a short grass surface on the prairies, a P-T coefficient of 0.65 was found to be appropriate for estimating the night-time vapour transfer. Monthly Energy Balance In order to investigate the seasonal trends, daily values of the terms in Eq. 1 were calculated for the three sites, and these were summed for each month of the study period. Table 1 presents the monthly totals of the energy balance terms, expressed in mm equivalent for the three sites, for the observation periods May through September, for the seasons 1994 through 1997. Also included are the observed precipitation values. Table 1. Monthly totals of the energy balance terms (mm equivalent) for the observation periods May through September, for 1994, 1995, 1996 and 1997. 37 Granger - Evaporation With the exception of the precipitation amounts, the respective values presented in Table 1 did not vary greatly from year to year. The average values of the monthly energy balance terms for the four study years were calculated, and these are presented graphically in Fig.1. The figure allows for a comparison of the typical energy balance conditions for the three land covers. Fig. 1 shows that the net radiation input at all sites peaks in June or July and drops off quickly in August and September. The amounts of radiation received at the three sites differs significantly, with the alpine site receiving the least and the forest site receiving the most net radiation. Although variations in cloud cover can account for differences in net radiation, the most significant factor affecting the net radiation input is the surface albedo; the observed average albedo values at the alpine, taiga and forest sites were 0.21, 0.18 and 0.09, respectively. Figure 1. The monthly energy balance, expressed in equivalent mm of evaporation, for the alpine, shrub taiga and forest sites for the period May through September. The values are the means of the study years 1994 - 1997. Partitioning of Energy: Latent and Sensible Heat The behavior of the latent and sensible heat terms appears to be somewhat more complex. Although the magnitude of the net radiation term drops off rapidly in August and September, the reduction in the latent and/or sensible heat term may be less abrupt. For the alpine site both the evaporation, E, and the sensible heat, H, follow the net radiation trend, indicating that the sparse vegetation at this site has very little effect on the partitioning of the incoming energy. The shrub taiga and forest sites show some divergence between the evapotranspiration and the sensible heat. At these sites, from June to September, the latent heat is greater than the sensible heat, with the difference being greatest for the forest site. 38 Wolf Creek Research Basin: Hydrology, Ecology, Environment To better demonstrate the partitioning of energy Figure 2 shows the fraction of the incoming net radiation used for the other energy balance components for the alpine, taiga and forest sites. The figure shows the average results for the four years of observation. The difference between the respective sites is quite visible. At the alpine site the latent and sensible heat terms are approximately equal throughout the snow-free season (Bowen ratio ≈ 1); the very sparse vegetation at this site cannot exert any significant control on the partitioning of energy and, with similar turbulent diffusivities the latent and sensible heat fluxes are similar. At the shrub taiga and forest sites, with significant vegetation, more energy is being diverted to evapotranspiration than to heating of the air; the difference between the two turbulent energy terms increases throughout the season at these sites, and the divergence is greatest for the forest where, for the month of September, approximately 70% of the incoming energy is being used for evapotranspiration. The average September Bowen ratios for the shrub taiga and forest sites are 0.7 and 0.5, respectively. Figure 2. The partitioning of the incoming energy, expressed as a fraction of the net radiation, for the alpine, shrub taiga and forest sites for the period May through September. The monthly values are the means of the study years 1994 - 1997. That the vegetated sites partition a greater amount of energy to evapotranspiration is not unusual; what is surprising, however, is the seasonal trend. Pomeroy et al.( 1996, 1997) showed that for the southern boreal forest the mature stands produced more evapotranspiration than cleared surfaces or regenerating stands; they showed that for the water-limited southern forest, the partitioning of energy between latent and sensible heat terms responded to the available moisture, that is, months with greater precipitation produced greater evapotranspiration. This appears (Fig. 2) not to be the case for the northern boreal forest vegetation, where the evaporative fraction increases throughout the 39 Granger - Evaporation growing season. Fig. 2 represents the average of the four study years; however, the same trend is evident for each year, with little response to variations in monthly precipitation. Soil Heat Flux The soil heat flux, as is the case for most situations, is the smallest term in the energy balance. Contrary to the radiation inputs, however, the soil heat fluxes are largest at the alpine site and least at the forest site. This is as expected, since the presence of surface cover and vegetation tends to reduce the contribution to soil heat storage. The mid-summer soil heat term is typically 10%, 6% and 3% of the net radiation term for the alpine, taiga and forest sites, respectively. These values (percentage of the net radiation contributing to soil heat) remain relatively constant throughout the growing season, dropping off only in September when the heat flux changes direction as soil refreezing begins. This seasonal trend is quite different from that observed at southern boreal forest sites (Pomeroy et al., 1996), where the soil heat fluxes are largest immediately after the snow melt, and decrease continuously throughout the growing season. Although there is some permafrost within the basin, none of the study sites has a permafrost subsoil. The soil heat flux regime under permafrost could be significantly different from those observed here. Water Use Pomeroy et al. (1996, 1997) suggested that the southern boreal forest has adapted its water use strategy to the dry conditions, increasing its evapotranspiration as water is made available; the observed partitioning of energy demonstrates the forests adaptation to local conditions. The northern forest is energy-limited; the peak energy supply (net radiation) occurs shortly after the beginning of the growing season and drops off quickly (Fig. 1), and the soil temperature regime limits the ability of the vegetation to transpire effectively early in the season. In order to maximize its productivity, the northern forest must maintain a relatively high water use; with a declining energy input, this results in a seasonal trend for the partitioning of energy as shown in Fig. 2. This may be further demonstrated by showing the relationship between evapotranspiration and precipitation inputs. Fig. 3 is a comparison of the average monthly values of the ratio of evapotranspiration to precipitation for the three sites; the 1994 data have been excluded because of missing values. Fig. 3 shows that for May all sites use more water than the amount supplied by precipitation during the period; all sites are making use of the snowmelt water. For the alpine site the ratio drops quickly to near unity. The shrub taiga utilizes 1.5 to 2 times the precipitation amount during the summer; the ratio declines steadily 40 Wolf Creek Research Basin: Hydrology, Ecology, Environment throughout the season. The forest site continues to utilize from 3.3 to 4.2 times the available precipitation throughout the growing season. In September, when defoliation occurs, the ratio drops significantly at all sites. Figure 3. The average monthly values of the ratio of evapotranspiration to precipitation for the Forest, Shrub Taiga and Alpine sites (1995 - 1997). Precipitation vs. Elevation The precipitation data provided here represents only three seasons, and as such is likely insufficient to derive specific relationships with elevation. However, the data demonstrate that the usually-accepted notion of precipitation increasing with elevation does not always hold. Although the three-year averages of the values from Table 1 show precipitation increasing with elevation, the individual monthly values generally do not necessarily show this trend. For example, in June 1996, the reversed trend is true, with precipitation decreasing with elevation. On a single event basis, the scatter is even greater. The data do suggest then that caution must be exercised when attempting to distribute precipitation over a mountainous basin based on valley bottom observations. Further analysis is required in order to develop useful relationships for distributing precipitation; such relationships will likely require some knowledge of storm type, storm track and topography. 41 Granger - Evaporation Summary Energy balance data collected at three representative sites (alpine tundra, shrub taiga and pine forest) in the Wolf Creek Research Basin during four snow-free seasons are presented and analyzed. The amounts of net radiation received at the three sites differs significantly, with the alpine site receiving the least and the forest site receiving the most net radiation. These variations are due to the large differences in the surface albedo. As expected, the soil heat fluxes are largest at the alpine site and least at the forest site. The seasonal pattern of partitioning of energy to latent and sensible heat fluxes does not appear to be governed by the seasonal pattern of precipitation, as is the case in the southern boreal forest where the relative contribution to the latent heat term is significantly reduced during the dry months. At the higher latitude sites the forest and shrub vegetation employ a water use strategy for maximum productivity that is adapted to the energy limited conditions encountered in the north. There appears to be no clear relationship between the precipitation at the three observation sites (the boreal forest in the valley bottom, the shrub taiga above the tree line and the high elevation alpine tundra), indicating that the application of an elevation correction factor to precipitation observations made at the climate station (valley bottom) could lead to significant errors in the estimation of the precipitation distribution within the basin. Relationships taking into account such factors as storm type, track and topography must be developed. Acknowledgements Funding assistance received through the Canadian GEWEX programme is gratefully acknowledged. The cooperation of Richard Janowicz and of his technical staff at the Water Resources Branch in Whitehorse is greatly appreciated. The collaboration provided by Dr. John Pomeroy and the proficient technical support provided by Newell Hedstrom and Dell Bayne, are also recognized and appreciated. 42 Wolf Creek Research Basin: Hydrology, Ecology, Environment References Bouchet, R.J., 1963. Évapotranspiration réelle et potentielle, signification climatique. IAHS Proceedings. Berkeley, CA, Symposium., Publ. No. 62: 134-142. Granger, R.J. and D.M. Gray, 1989. Evaporation from natural non-saturated surfaces. J. Hydrology, 111: 21-29. Granger, R.J., 1991. Evapotranspiration from nonsaturated surfaces. Ph.D. Thesis. Dept. of Agricultural Engineering, University of Saskatchewan, 141p. Penman, H. L., 1948. Natural evaporation from open water, bare soil and grass. Proc. R. Soc. London, Ser.A, 193: 120-145. Pomeroy, J.W., R.J. Granger, N. Hedstrom, B. Toth, J. Parviainen and A. Pietroniro, 1996. Quantification of Hydrological Pathways in the Prince Albert Model Forest, 1995-1996 Annual Report. Environment Canada (NHRI) Report to the Prince Albert Model Forest Association. NHRI Contribution Series CS-96007. 60pp. Pomeroy, J.W., R.J. Granger, A. Pietroniro, J.E. Elliott, B. Toth and N. Hedstrom, 1997. Hydrological Pathways in the Prince Albert Model Forest, Final Report to the Prince Albert Model Forest Association. Environment Canada, NHRI Contribution Series No. CS-97004. 154p + appendices. Priestley, C.H.B. and R.J. Taylor, 1972. On the assessment of surface heat flux and evaporation using large-scale parameters. Monthly Weather Rev., 100: 81-92. 43 Granger - Evaporation 44
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