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Riccardo Rigon
IlSole,F.Lelong,2008,ValdiSella
Solar Radiation
Coping with terrain
R. Rigon
Finally the residual radiation hits the terrain
The terrain is not a plane
but it is inclined. Therefore,
besides correcting radiation
for latitude, longitude and
hour, it is necessary to
account for slope and
aspect
2
Hitting the terrain
R. Rigon
In the presence of topographic surfaces
In the northern hemisphere, slopes that face South receive a greater insolation
and, therefore, the water in the soil evaporates more quickly or the snow melts
faster. Slopes with differing aspects are often characterized by different species
and densities of plants and trees.
3
Hitting the terrain
R. Rigon
Projection of radiation onto an
inclined surface
AfterCorripio,2003
First we calculate the normal to the surface 4
Hitting the terrain
R. Rigon
⇧nu =
1
|⇧nu|
⇧
⇧
⇧
⇧
⇤
1/2 (z(i,j) z(i+1,j) + z(i,j+1) z(i+1,j+1))
1/2 (z(i,j) + z(i+1,j) z(i,j+1) z(i+1,j+1))
l2
⇥
⌃
⌃
⌃
⌃
⌅
where z are the elevations of the four points used and l2 is the are of the
cell - of side l.
Projection of radiation onto an
inclined surface
Unit normal vector:
5
AfterCorripio,2003
Hitting the terrain
R. Rigon
AfterCorripio,2003
6
Representation of the vector normal to the surface of Mount Bianco
Hitting the terrain
R. Rigon
AfterCorripio,2003
Projection of radiation onto an
inclined surface
And we compare with the solar vector, indicating the direction of the Sun 7
Hitting the terrain
R. Rigon
8
⌥s = ⇤
sin ⇥ cos
sin ⇤ cos ⇥ cos cos ⇤ cos
cos⇤ cos ⇥ cos + sin ⇤ sin
⇥
⌅
Projection of radiation onto an
inclined surface
Where all the quantities were already defined previously
Hitting the terrain
R. Rigon
AfterCorripio,2003
Projection of radiation onto an
inclined surface
9Then we calculate the angle between the sun vector and the normal
s
Hitting the terrain
R. Rigon
We can define then the angle
of solar incidence
AfterCorripio,2003
Projection of radiation onto an
inclined surface
10
s
Hitting the terrain
R. Rigon
Projection of radiation onto an
inclined surface
Angle of solar incidence
cos s = ⌅s · ⌅nu
⇧nu =
1
|⇧nu|
⇧
⇧
⇧
⇧
⇤
1/2 (z(i,j) z(i+1,j) + z(i,j+1) z(i+1,j+1))
1/2 (z(i,j) + z(i+1,j) z(i,j+1) z(i+1,j+1))
l2
⇥
⌃
⌃
⌃
⌃
⌅
⌥s = ⇤
sin ⇥ cos
sin ⇤ cos ⇥ cos cos ⇤ cos
cos⇤ cos ⇥ cos + sin ⇤ sin
⇥
⌅
11
Hitting the terrain
R. Rigon
s = cos 1
nu.z
Aspect (from the North anti-clockwise)
Projection of radiation onto an
inclined surface
Slope
The above angles needs to be compared with those of the terrain:
12
Hitting the terrain
R. Rigon
13
Projection of radiation onto an
inclined surface
Remarkably the form of formula for the incident radiation is the same that
for a flat surface when the projection angle is accounted:
Hitting the terrain
R. Rigon
Solar radiation transmitted to the ground under
clear sky conditions
Therefore, for the direct
shortwave radiation:
Corripio,2002
14
S
as, it was before
Hitting the terrain
R. Rigon
15
However, it is not just matter of light but also of
shadows
Hitting the terrain
R. Rigon
Incident radiation
Topographic effects: shading
16
More schematically
shadow
light
Hitting the terrain
R. Rigon
Incident radiation
Topographic effects: shading
17
More schematically
light
shadow
Hitting the terrain
R. Rigon
Incident radiation
DetailsinCorripio,2003
18
Therefore the direct solar radiation must be corrected to include shading
Hitting the terrain
R. Rigon
sky view factor
diffuse
radiation due to
Rayleigh
scattering
diffuse
radiation due to
aerosols
diffuse
radiation due
multiple
scattering
What about diffuse radiation ?
Topographic effects: angle of view
19
Hitting the terrain
R. Rigon
Incident radiation
Topographic effects: angle of view
20
Any point in a rugged landscape see just a part of the sky sphere. Its fraction
says which portion of the sky contribute to diffuse shortwave radiation.
Hitting the terrain
R. Rigon
Incident radiation
Topographic effects: angle of view
21
Different points view a different sky
Hitting the terrain
R. Rigon
22
The sum
Hitting the terrain
R. Rigon
AfterCorripio,2003
23
Now it really hits the terrain
and, in part, it is reflected away
Hitting the terrain
R. Rigon
AfterCorripio,2003
24Insolation received by Mont Blanc at Spring Equinox
Finally a map
Hitting the terrain
R. Rigon
Typical albedo values
25
http://en.wikipedia.org/wiki/Albedo
Albedo
R. Rigon
Typical albedo values
26
http://en.wikipedia.org/wiki/Albedo
Albedo
R. Rigon
51
The percentage of radiation that is reflected (reflectance) depends on
wavelength of the radiation, and on the geometry, nature, and structure
of the surface under investigation.
Spectral Signature (or Response)
27
Spectral response
R. Rigon
•In the case of solar radiation, the spectral signature is defined
as the reflectance of the surface in function of the wavelength.
28
Spectral response
R. Rigon
29
•Every type of surface can be statistically characterised by a spectral signature.
Spectral response
R. Rigon
•The spectral signature of a specific element of a territory will
vary due to the variability of local environmental factors.
•Given a certain type of ground cover, static elements, such as
slope and exposition, and dynamic elements, such as surface
ground humidity, the phenological state of the vegetation, the
atmospheric transparence, etc., will cause variations in the
spectral signature curve.
Factors
30
Spectral response
R. Rigon
Radiation that hits the terrain, heats it.
Or causes changes of phase
water to vapor
ice to water
31
Spectral response

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6 h-coping withterrain

  • 2. R. Rigon Finally the residual radiation hits the terrain The terrain is not a plane but it is inclined. Therefore, besides correcting radiation for latitude, longitude and hour, it is necessary to account for slope and aspect 2 Hitting the terrain
  • 3. R. Rigon In the presence of topographic surfaces In the northern hemisphere, slopes that face South receive a greater insolation and, therefore, the water in the soil evaporates more quickly or the snow melts faster. Slopes with differing aspects are often characterized by different species and densities of plants and trees. 3 Hitting the terrain
  • 4. R. Rigon Projection of radiation onto an inclined surface AfterCorripio,2003 First we calculate the normal to the surface 4 Hitting the terrain
  • 5. R. Rigon ⇧nu = 1 |⇧nu| ⇧ ⇧ ⇧ ⇧ ⇤ 1/2 (z(i,j) z(i+1,j) + z(i,j+1) z(i+1,j+1)) 1/2 (z(i,j) + z(i+1,j) z(i,j+1) z(i+1,j+1)) l2 ⇥ ⌃ ⌃ ⌃ ⌃ ⌅ where z are the elevations of the four points used and l2 is the are of the cell - of side l. Projection of radiation onto an inclined surface Unit normal vector: 5 AfterCorripio,2003 Hitting the terrain
  • 6. R. Rigon AfterCorripio,2003 6 Representation of the vector normal to the surface of Mount Bianco Hitting the terrain
  • 7. R. Rigon AfterCorripio,2003 Projection of radiation onto an inclined surface And we compare with the solar vector, indicating the direction of the Sun 7 Hitting the terrain
  • 8. R. Rigon 8 ⌥s = ⇤ sin ⇥ cos sin ⇤ cos ⇥ cos cos ⇤ cos cos⇤ cos ⇥ cos + sin ⇤ sin ⇥ ⌅ Projection of radiation onto an inclined surface Where all the quantities were already defined previously Hitting the terrain
  • 9. R. Rigon AfterCorripio,2003 Projection of radiation onto an inclined surface 9Then we calculate the angle between the sun vector and the normal s Hitting the terrain
  • 10. R. Rigon We can define then the angle of solar incidence AfterCorripio,2003 Projection of radiation onto an inclined surface 10 s Hitting the terrain
  • 11. R. Rigon Projection of radiation onto an inclined surface Angle of solar incidence cos s = ⌅s · ⌅nu ⇧nu = 1 |⇧nu| ⇧ ⇧ ⇧ ⇧ ⇤ 1/2 (z(i,j) z(i+1,j) + z(i,j+1) z(i+1,j+1)) 1/2 (z(i,j) + z(i+1,j) z(i,j+1) z(i+1,j+1)) l2 ⇥ ⌃ ⌃ ⌃ ⌃ ⌅ ⌥s = ⇤ sin ⇥ cos sin ⇤ cos ⇥ cos cos ⇤ cos cos⇤ cos ⇥ cos + sin ⇤ sin ⇥ ⌅ 11 Hitting the terrain
  • 12. R. Rigon s = cos 1 nu.z Aspect (from the North anti-clockwise) Projection of radiation onto an inclined surface Slope The above angles needs to be compared with those of the terrain: 12 Hitting the terrain
  • 13. R. Rigon 13 Projection of radiation onto an inclined surface Remarkably the form of formula for the incident radiation is the same that for a flat surface when the projection angle is accounted: Hitting the terrain
  • 14. R. Rigon Solar radiation transmitted to the ground under clear sky conditions Therefore, for the direct shortwave radiation: Corripio,2002 14 S as, it was before Hitting the terrain
  • 15. R. Rigon 15 However, it is not just matter of light but also of shadows Hitting the terrain
  • 16. R. Rigon Incident radiation Topographic effects: shading 16 More schematically shadow light Hitting the terrain
  • 17. R. Rigon Incident radiation Topographic effects: shading 17 More schematically light shadow Hitting the terrain
  • 18. R. Rigon Incident radiation DetailsinCorripio,2003 18 Therefore the direct solar radiation must be corrected to include shading Hitting the terrain
  • 19. R. Rigon sky view factor diffuse radiation due to Rayleigh scattering diffuse radiation due to aerosols diffuse radiation due multiple scattering What about diffuse radiation ? Topographic effects: angle of view 19 Hitting the terrain
  • 20. R. Rigon Incident radiation Topographic effects: angle of view 20 Any point in a rugged landscape see just a part of the sky sphere. Its fraction says which portion of the sky contribute to diffuse shortwave radiation. Hitting the terrain
  • 21. R. Rigon Incident radiation Topographic effects: angle of view 21 Different points view a different sky Hitting the terrain
  • 23. R. Rigon AfterCorripio,2003 23 Now it really hits the terrain and, in part, it is reflected away Hitting the terrain
  • 24. R. Rigon AfterCorripio,2003 24Insolation received by Mont Blanc at Spring Equinox Finally a map Hitting the terrain
  • 25. R. Rigon Typical albedo values 25 http://en.wikipedia.org/wiki/Albedo Albedo
  • 26. R. Rigon Typical albedo values 26 http://en.wikipedia.org/wiki/Albedo Albedo
  • 27. R. Rigon 51 The percentage of radiation that is reflected (reflectance) depends on wavelength of the radiation, and on the geometry, nature, and structure of the surface under investigation. Spectral Signature (or Response) 27 Spectral response
  • 28. R. Rigon •In the case of solar radiation, the spectral signature is defined as the reflectance of the surface in function of the wavelength. 28 Spectral response
  • 29. R. Rigon 29 •Every type of surface can be statistically characterised by a spectral signature. Spectral response
  • 30. R. Rigon •The spectral signature of a specific element of a territory will vary due to the variability of local environmental factors. •Given a certain type of ground cover, static elements, such as slope and exposition, and dynamic elements, such as surface ground humidity, the phenological state of the vegetation, the atmospheric transparence, etc., will cause variations in the spectral signature curve. Factors 30 Spectral response
  • 31. R. Rigon Radiation that hits the terrain, heats it. Or causes changes of phase water to vapor ice to water 31 Spectral response