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October 30, 2017 | Author: Anonymous | Category: N/A
Short Description
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE. 10. Air column. (3) Irradiance per air column ......
Description
TherMap Thermal Maps
Use of Topographic Radar Scans to Identify Thermal Hotspots in Alpine Areas
Contents
History and present state of thermal maps The TherMap approach Topography – Irradiance – Temperature Thermal Take-Off Spots
Model validation Conclusions
May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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“Flashlight Analogy” of 1955
Hans Nietlisbach
May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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Example of an Existing Thermal Map
Thermikkarte Deutschland Considers neither daytime nor season
May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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Topographic Approach by TherMap Topographic data model
Topography of a region
Date and daytime
Irradiance map (W/m2)
Surface properties
Temperature map (heating effect)
Regional meteorology
Thermal map (?)
May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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A. Topography SRTM 90 m Satellite Radar Data
These are tables indicating the elevation of the surface of the earth every 90 Topographic meters Topographic Map Map Example: Example: Elevation Elevation Map Map
Used to generate computed maps
May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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B. Irradiance The intensity of solar radiation (W/m2)
at a given location, date and time
PVGIS © European Communities, 2002-2006 Šúri M., Huld T.A., Dunlop E.D. (2005). PVGIS: a web-based solar radiation database for the calculation of PV potential in Europe. International Journal of Sustainable Energy, 24, 2, 55-67.
May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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(1) Basic Irradiance = Projection of solar vector on normal vector
Normal vector
Solar vector
Parabolic approximation line
Tangent
May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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(2) Irradiance is diminished as light penetrates the atmosphere ~1.3 kW/m2 before entering atmosphere
Depending on • Solar elevation • Altitude • Turbidity
Present TherMap assumption: 12 km visibility (for turbidity) In reality locally and seasonally variable May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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(3) Irradiance per air column is scaled by the slope of the surface (solar pannel)
Sun
Air column
Irradiated surface
IIhh = = IIss // cos cos αα Horizontal surface
May 06
α
Slope angle
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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Example:
May 06
Irradiance, Jura-Gruyères/CH, May 6, 1100 MEZ
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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C. Temperature Temperature increase due to cumulative effect of solar irradiation minus radiation losses
Solar Engineering Handbook Part 2, “Temperature Theory”, ed. 2003, Meteonorm, http://www.meteotest.ch/en/mn_dl?w=ber
On a sunny day the Temperature is peaking about 2 hours after the Irradiance peak May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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Irradiance - Temperature
Temperature: Approximation by a timephased smoothing model Irradiance 0.6 0.5 0.4 0.3 0.2
Smoothing model with smoothing factor a = 0.1 to 0.6
0.1 6
12
18
24
Irradiance - Temperature
Time of day (hour)
6.00
8.00
10.00
12.00
14.00
16.00
18.00
20.00
Present best fit: Smoothing model with time-phased smoothing factor a = 0.2 x 0.9(hr-12)
Hour
May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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Effects diminishing Temperature increase
y t i s n e d h n t i o i w t a s et she g Ve ini d im p e ! s lo
Albedo of snow covered surfaces (seasonal)
Forest belt from 900 – 1500 m
Seasonally climbing and descending vegetation May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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Example:
Temperature, Valais/CH, May 6th
1100h 1300h MEZ 1700hMEZ MEZ 1500h MEZ
May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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Thermal Take-Off Spots (von Kalckreuth’s rule) Thermals climb along slope until angle drops below 30 degrees
May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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Example: Take-Off Spots on Overlay Temperature Map (Sisteron May 6, 1300 MEZ)
May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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Model Validation
Expert advice Overlayed IGC logfiles of flights on days with few and high clouds unstable atmosphere (temperature increase leading to thermals) (if possible) comments by the pilots Regions: Alps, Jura, Black Forest/DE
May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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Validation: Net Vario Vario Net Vario Speed
Polar curve
Actual Vario
Actual speed
May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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June 28 Engadin June 28
Validation Examples
June 28
May 06
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Conclusions
TherMap model seems to be valid for topographically highly differentiated areas, such as the Alps Mixed results for topographically smoother regions, such as the Jura:
(+) Irradiance (~) Temperature
Not sufficient for still smoother regions
May 06
OK
~
X
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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Note on Irradiance Maps in “Smooth” Areas Thermal map
The Thesimilarity similarity would wouldseem seemto to justify justifyfurther further research research
Irradiance map
May 06
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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Next Steps
Internet publication: Maps, forum, services R&D on
May 06
Secondary IR effects (lakes, ice, vegetation, satellite IR scans) Variation of turbidity Temperature model Secondary aerodynamic effects Refined flight tracking (wind drift, ground tracks) Extention to non-Alpine regions
d n a Help e c i v d A ! e m o c l e W
B. Sigrist - TherMap OSTIV 2006, Eskilstuna/SE
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Thank You
May 06
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