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Energy Budget at land surface

LE. LW. . SR. E s /t. The surface layer. Energy Budget at land surface. Energy budget of a surface layer without vegetation:. Ch. 5 in Garratt’s text, reference: Hartmann’s global physical climate. LE. LW. . SR. The surface layer.

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Energy Budget at land surface

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  1. LE LW  SR Es/t The surface layer Energy Budget at land surface Energy budget of a surface layer without vegetation: Ch. 5 in Garratt’s text, reference: Hartmann’s global physical climate

  2. LE LW  SR The surface layer • Under steady-state and when the energy storage is small, the energy budget of a land surface layer can be simplified to • Rn=LE-H because usually Fout << Rn, LE, H • Factors left out but can be important for some locations and periods: • Fraction of solar energy that is stored in the chemical bones formed during photosynethesis, can reach 5% during growing period (?); • Heat released by oxidation of biological substance as in biological decade or biomass burning; • Heat released by fossil fuel burning or nuclear power generation (e.g., big urbane areas); • Convection of the kinetic energy of winds into thermal energy; • Heat transferred by precipitation, especially when precipitation is much cooler than the surface; • Geothermal energy released in hot springs, earthquakes and volcanoes. These factors are generally unimportant globally.

  3. Surface with vegetation: • Vegetation will contributes to or dominate the surface albedo. The top of the surface layer is at the canopy level. Energy divergence and energy storage in the canopy layer can be significant, especially on scale shorter than daily. Sensible, latent heat of the air column & change of heat content of vegetation

  4. Physical Properties of Soil organics minerals water ice air Cs (Jm-3K-1)= rs cs fs + rc cc fc + rw cw fw + ri ci fi + ra ca fa Soil is a mixture of several materials, each with quite different physical properties heat capacity of soil density volume fraction heat capacity

  5. For a periodic forcing of period t, e.g., diurnal, seasonal, the response of T(z) is also periodic, but damped and delayed with depth relative to surface forcing. • Soil temperature and heat flux: • Heat flux • Soil temperature:

  6. 6am 10 pm 6 pm 10am 12, 2 pm • Why?

  7. 6am 10 pm 6 pm 10am 12, 2 pm • For 2s~ 5 x 10-7 m2 s-1, • diurnal cycle,  1 day, D~0.1 m • annual cycle, year, D~1.5 m • glacial-interglacial, years, D~150 m • In reality, changes are not pure sinusoidal, use • 25 K diurnal cycle at 0.5 cm, Max T around 2 PM • Only 6 K diurnal range at 10 cm’, Max T about 6 PM: Damped and delayed with depth • Negligible diurnal cycle at 50 cm

  8. LE LW  SR The surface layer The surface fluxes: The net radiative flux (Rn) The latent flux (LE) The sensitive flux (H) Rn: The Radiative fluxes • Rn,o = Solar flux - longwave flux = SR(1-s) + (1-s)LWDN,o- sT4 • s: surface albedo • s: surface emissivity. If the same frequencies

  9. The surface albedo, emissivity changes with surface type, wave frequency. • Surface Albedo: s,, the ratio of reflected vs. incoming solar flux (integrated over all direction of the hemisphere). • Total surface solar albedo: s integrates for all solar spectrum

  10. Global land surface albedo:

  11. Surface Albedo (percent) • Snow and ice brightest • Deserts, dry soil, and dry grass are very bright • Forests are dark • Coniferous (cone-bearing) needleleaf trees are darkest

  12. Spectrum dependent Land-Surface Albedo • Strong wavelength dependence over vegetated land • Plants absorbs strongly (upto 90%) of the solar radiation between 0.3-0.7 mm for photosynthesis (photosynethetically active radiation or PAR), reflect strongly in near-IR to avoid heating. • Total albedo is a weighted mean over wavelengths

  13. Seasonal change of surface albedo for total visible solar and PAR radiation: Left: true color albedo Right: albedo for PAR

  14. Solar radiation at the canopy: • Visible solar (VIS) is less reflected and can penetrate deeper in canopy; whereas the near infrared solar (NIR) is more reflected by canopy; • Thus, nir/vis with depth below top of the plants; • Larger difference between nir and vis, i.e., the large NDVI (Normalized Differential Vegetation Index), indicates large biomass of the plants. • Cavities and different leaf orientations of the canopy can lead to a lower canopy albedo compared to a single leaf. • The absorption of PAR depends on the leaf area index (LAI).

  15. The leaf area index, LAI: • LAI: The ratio of total canopy leaf surface area vs. horizontal ground area covered by canopy. • Global annual minimum and maximum LAI. • Tropical forests: > 4, 5 • Grassland:≤ 1

  16. Asner et al. 2003: Global synthesis of LAI(Global Ecology & Biogeography, 12, 191-205)

  17. Reading and discussion: • Land surface albedo: • Tues: • Charney 1977: albedo effect on drought • Sailor 1995: albedo effect on urban climate • Thurs: • We will select and discuss 2 out 3 papers: • Gao, F., C. Schaaf, A. Strahler, A. Roesch, W. Lucht, and R. Dickinson, The MODIS BRDF/Albedo Climate Modeling Grid Products and the Variability of Albedo for Major Global Vegetation Types, J. Geophys. Res., 110, D01104, doi:10.1029/2004JD00519, 2005. • Tsvetsinskaya et al. 2002: link between surface albedo to soil and rocks in N. African and Arabian desert areas • Moody et al: 2007: observed albedo changes due to snow on vegetation, Remote sensing of environment, vol 111, issues 2-3, Nov. 2007, page 337-345.

  18. Extra reading if you are interested in:

  19. Infrared Emissivity

  20. Solar radiation: • SRs,dn=Itopa sin •  sun elevation, Itop: solar irradiance reaches the top of the atmosphere • Direct and diffused:

  21. How does vegetation-BLCu interact? • Normalized downward solar radiation: K/ KTOA=a + bC Where K : downward solar at surface, KTOA : downward solar at top of atmosphere C: cloud cover Normalized std K/ KTOA: are often caused by diffused radiation from side of BLCu Most of the samples come from BLCu cases North central Massachusetts: 54N, 72.18W, Freedman et al. 2001

  22. Z”+dz” Tj(z”) dm Z” • Lougwave: m Z” Ti(z”) dm Z”+dz” LWDN,o To4

  23. Radiation Budget: Diurnal Cycle • Net solar follows cos q • LW fluxes much less variable (esT4) • LW up follows surface T as it warms through day • LW down changes little • LW net opposes SW net • Rs positive during day, negative at night Canadian Prairie Late July (no clouds)

  24. Effects of Clouds Clouds add variance, and shift radiation load from direct to diffuse (nondirectional)

  25. Surface ET: • Surface ET is controlled by multiple processes, • evaporation from bare soil and leaf, • transpiration from leaf. 

  26. Evaporation over wet canopy and soil: • Similar to pan-evaporation or potential (maximum ET). Convenient with surface meteorological obs.

  27. Aerodynamic resistance (refresh): • An alternative to represent drag coefficients, convenient for field meteorology and plant physiology analog to Ohm’s law (resistanceXcurrent=potential difference)

  28. ET from dry vegetation: • For close canopy (LAI>1)

  29. ET for open canopy: • Combined foliage and sub-canopy ET, and evaporation from the open areas between the vegetation. The Penman-Monteith equation.

  30. Characteristics of the hypothetical reference crop Typical presentation of the variation in the active (green) Leaf Area Index over the growing season for a maize crop

  31. ET over dry (unsaturated) surface: • Eo is determined by surface soil relative humidity. rh=qo/q*(To) • Surface soil moisture is determined by soil moisture flux (without rain) and hydraulic lifting of roots.

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