Neusiedler See project

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Young Authors Paper Analysis of ALS data and products in the Neusiedler See project Maja Bitenc

Objectives Technology of ALS Project Neusiedler See. Analyse of DTM quality Analyse of intensity Conclusion Outline 2

Objectives Getting to know the ALS. Acquiring practical experiences. DTM Quality control of the project Neusiedler See (sigmadtm.exe). Analising the intensity measurements of the project Neusiedler See. 3

Basics of ALS ALS mission o Data acquisition o Laser light o Moving of the laser beam Postprocessing o 3D coordinates Computation of the results o Digital Terrain Model (DTM) o Digital Surface Model (DSM) Application 4

Project Neusiedler See-Seewinkel Seewinkel Project regions 1 4 2 3 Objactives: renaturalization of the natural basisn Aim: modeling high resolution and accuratedtm fot hydrological analysis. 5

Data acquisition ALS mision Company: TopScan Fliing date: 24. and 25. 11. 2004 Area: ~ 250 km² Number of strips: 57 Number of points: 1,05 miljarde Density: 1,5 točke na m² Measurement sistem: ALTM 2050 Digital camera: Emerge DSS Terrestrial measurements Areas: 12 kontrolnih mest Measurement basis: GPS mreža Method: tachimetry Expected accuracy: ± 3 cm 6

Terrestrial measurements Example: surveyed roofs in control area 10 7

Postprocessing Polar coordinates (R, α) Orientation Position Calibration data (dx, dy, dz, δω, δφ, δκ) Integration of DGPS and INS Orientation parameters (X o, Y o, Z o, ω, φ, κ ) GEOREFERENCING Time synchronization 3D point coordinates (X, Y, Z) WGS84 8

Skrbno georeferenciranje Polar coordinates (R, α) Orientation Position Calibration data (dx, dy, dz, δω, δφ, δκ) Tie points Tie patches (searching in the overlapping area) FINE GEOREFERENCING Simultaneous block adjustment of strips Control points Control patches (terrestrial measurements) Adjusted 3D point coordinates (X, Y, Z) WGS84 9

The DTM computation Iterative robust interpolation. Profile Weight function 10

Processing the measurements Digital terrain model calculation. Hierarchic iterative robust interpolation (SCOP++) 11

Global quality parameters σ z DTM quality control 6 [ cm] = ± + 30 tanα Where: n point density per square meter; tan(α) terrain slope; 6 in 30 experimentally computed parameters n Local quality parameters The method for the derivation of the height accuracy of each grid point. (sigmadtm.exe) o Used also for existing DTM. o independent of the interpolation method. o Grid resolution. o Attractive visualization (SCOP++). o Input data: original points, DTM. o Results: 5 digital models of quality parameters. 12

The local paramaters and visualization Minimum distance between each grid point and its nearest original point. Maximum main curvature. Height accuracy of original points σ0,d. Weight coefficient qa0. Height accuracy of the DTM σˆ DMR = σ 0.d q a 0 13

Comparison of local parameters 1/2 1. Schilf 2. Village 3. Vineyard 4. Field 5. Wood 14

Comparison of local parameters 2/2 1. Schilf 2. Village 3. Vineyard 4. Field 5. Wood 15

Intensity measurements analyze ALS measurements: polar coordinates, position, orientation, intensity. Influencing factors. o Laser scanner o atmosphere o target Definition; relation between emitted and received strength of laser wavelength. 16

Identical points Measured intensity: P ρ I m r P t = * konst. 2 R Intensity of identical points: I m1 = I m2 17

Normalization Δ I m = a * ΔR + b Relative normalization: 1. possibility : I 2 (2. strip is master) n I1 I1 = I m,1 + ΔI( ΔR) 2. possibility : I 1 (1. strip is master) n I 2 I 2 = I m,2 ΔI( ΔR) 18

Normalization results 19

Classification Example: classification of green fields (meadows). 20

Conclusion DTM quality control o The DTM of Neusiedler See is very accurate. o The planimetric control of the DTM. o The calculation and the visualization of parameters is simple. o Data layers. Thank you for your Intensity measurement analyze attention! o Constant shift in measurements height of the flight. o Classification is not possible. Just lidar data do not suffice. o Potentially useful information about the surface. o Influencing factors. o Intensity dependency. o Different applications of intensity. 21