Opened 15 years ago
Last modified 6 years ago
#899 assigned enhancement
Better documentation and examples for i.eb.* and related modules requested
Reported by: | huhabla | Owned by: | ychemin |
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Priority: | minor | Milestone: | 7.6.2 |
Component: | Docs | Version: | svn-trunk |
Keywords: | imagery, i.eb.*, r.sunhours | Cc: | grass-dev@…, ychemin |
CPU: | All | Platform: | All |
Description
I would like to request a major documentation update for the new i.eb.* and related modules (i.sunhours, i.albedo, ...?). It would be great if we can see:
- More detailed description of the specific usage for each module with examples
- Better description of several abbreviations (eb, ETa, ETo, ETrF)
- Knowledge transfer from the pointed literature into the module documentation, it was hard for me to find online available referred literature.
- Integrative examples how to combine all these modules in a meaningful manner, this will make work much easier and will prevent errors in handling those modules.
- Adding i.eb.* introduction and usage to the imagery introduction page
- Several modules are referred, but they are only available in the addon wiki, if these modules are important, maybe they should go direct into grass7. If not, alternative processing method should be documented?
Many thanks in advances Soeren
Change History (15)
comment:1 by , 11 years ago
Cc: | added |
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Owner: | changed from | to
Status: | new → assigned |
comment:2 by , 11 years ago
Keywords: | r.sunhours added; i.sunhours removed |
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follow-up: 4 comment:3 by , 11 years ago
Some potential material coming up for the EGU 2014 in
http://svn.osgeo.org/grass/grass-promo/grassposter/2014_EGU_WD_Landscape/
comment:4 by , 10 years ago
Replying to neteler:
Some potential material coming up for the EGU 2014 in
http://svn.osgeo.org/grass/grass-promo/grassposter/2014_EGU_WD_Landscape/
And I think there is a little bit more in
http://svn.osgeo.org/grass/grass-promo/grassposter/2015_EGU_G7_PeerReview_SciPlatform/
comment:5 by , 9 years ago
Cc: | added |
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Component: | Imagery → Docs |
comment:6 by , 9 years ago
Milestone: | 7.0.0 → 7.0.5 |
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comment:7 by , 8 years ago
Milestone: | 7.0.5 → 7.3.0 |
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comment:10 by , 7 years ago
Milestone: | 7.4.1 → 7.4.2 |
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comment:12 by , 6 years ago
AFAICT, all i.eb.* modules in core have still a very minimal description and they all lack examples. These latter are pretty difficult to include (for someone not in the field) without a proper description of what the module does and what the parameters mean or how they are supposed to be obtained.
Maybe an i.eb general manual could give the basics of the process and then each module describe the specifics.
comment:13 by , 6 years ago
Milestone: | 7.4.2 → 7.6.0 |
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All enhancement tickets should be assigned to 7.6 milestone.
The radiation is coming from the planet's star, Earth has around 1800 W/m2 of incoming radiation from the sun (also called irradiance) at exo-atmospheric altitude.
Atmospheric transfer of irradiance is subject to atmosphere particles interactions, scattering, diffraction, reflection, etc.
When reaching the planetary surface, is it partially reflected in the shortwave by Albedo. Surface Albedo is the integrated 0.3-3 micro-meters reflectance, it reflects the shortwave energy coming from the sun by 5% on oceans, 15-25% on vegetation, 35-40% on sand/desert/beach, 60-80% on snow/clouds, roughly. This energy fraction is returned to atmosphere for complex interaction with gas particles again before leaving the atmosphere altogether.
As for the shortwave surface balance, the energy is also received in the longwave, but interacts with the grey-body characteristics of the surface elements. The blackbody to greybody fraction is ruled by emissivity, a hidden component in the thermal spectrum (search for Temperature-Emissivity Separation algorithms). On Earth, emissivity is always above 0.9 (mostly 0.96-0.98). The Stefan-Boltzman equation is dealing with blackbody energy, and multiplying it by Emissivity transforms it to greybody energy emitted.
Together, shortwave and longwave energy balance provide with the net radiation balance at the surface of the planetary body. This crucial term is the total energy available for thermodynamic fluxes to act on the surface of the planet. On a planet like Earth where there is a triple phase of a given molecule (H20, in gas, liquid, solid), energy available is used to transfer phases from lower energy to higher energy (sublimation, liquefaction, evaporation). Thermal transfers also happen as conduction (soil, rocks) and convection (atmosphere, oceans). The i.eb.* modules and models deal with conduction (i.eb.g0, for thermal conduction in soils), convection (i.eb.h_* especially, for thermal convection in atmosphere) and by residual method estimate the energy left for evaporation processes (i.eb.evapf, i.eb.eta are examples).
i.evapo.* modules/models are integrated models, from the oldest (Penman-Monteith i.evapo.pm, Priestley-Taylor i.evapo.pt, Hargreaves i.evapo.mh, etc) that are not based on energy balance, but are computing some form of evapotranspiration (ETo: Evapotranspiration for a reference of 20cm well-watered grass, see FAO no56 report of Richard Allen) to newer that area in some form or another linked to thermal processes (i.evapo.senay: uses a thermal index), biome thermal processes (i.evapo.zk: global model based on typical info from biomes Albedo/soil heat flux) or more thermodynamic processes (i.evapo.potrad: potential ET if not water stress, based on astronomical equations only). Most developed thermodynamic models are TSEB (i.evapo.tseb: Two Source Energy Balance, Schmugge, Kustas, etc., 2000), SEBS (i.evapo.sebs: Zhu et al, 2002), SEBAL (i.eb.h_SEBAL95, i.eb.g0, i.eb.evapfr, i.eb.eta: Bastiaanssen et al, 1998), and some newer models like RESET and others. The list of models using thermodynamic principles is large now, and any willing to submit a code for any of them is most welcome.