Full text: Technical Commission III (B3)

   
  
   
  
  
  
  
    
  
  
  
   
   
    
  
    
   
   
  
   
  
    
   
   
  
   
   
  
    
  
  
    
      
  
Figure 4: Images used for the radiance retrieval, from left and 
right cameras, for 6 vehicle locations (all images displayed with 
the same settings). 
the sky radiance coming from all points of the upper hemisphere, 
using images acquired by a ground-based mobile-mapping vehi- 
cle, with an accurate geolocation, but affected with radiometric 
artifacts. The method aims at working for all weather conditions. 
This problem is ill-conditioned since the true signal due to sky 
radiance and the noise signal due to radiometric artifacts cannot 
be demixed. 
3 SKY RADIANCE ESTIMATION 
In this section, we propose two different approaches to estimate 
the radiance map from the images: aggregation of pixels detected 
as sky (including the clouds), and estimation parametric model 
with blue sky pixels (avoiding clouds). These two methods can 
be mixed in order to reduce the influence of artifacts and try to 
enhance the accuracy of the sky radiance estimation. The corre- 
sponding results are presented in section 4.1. 
3.1 Extraction and aggregation of sky pixels 
The first task is to extract the pixels that see the sky in the images, 
in order to set them apart from pixels of building or vegetation. 
We use simple thresholds on color values, set by experiments on 
the data set. These thresholds must lead to a good balance be- 
tween accepting clouds and rejecting highly illuminated walls. 
The reflexions on cars are not a problem because pixels below 
the horizon are not used, but reflexions on windows are usually 
above the vehicle; a morphological filtering is used to remove 
most of the small areas detected among the buildings. The thresh- 
olds used are as follows, where the Cmin threshold depends on the 
camera response and its bit depth : 
R—B 
MAX(R,G,B) — MIN(R,G.B) 
  
<c, and MAX(R,G,B) > Cmin 
(1) 
    
International Archives of the Photogrammetry, Remote Sensing and Spatial Information Sciences, Volume XXXIX-B3, 2012 
XXII ISPRS Congress, 25 August — 01 September 2012, Melbourne, Australia 
    
a) b) C) 
Figure 5: Result of sky--clouds (a) and blue sky (b) detection. 
The main errors remaining are overdetection of large windows 
and of bright walls above the horizon, as well as a lack in detec- 
tion of dark clouds. The sky areas affected by strong bloom are 
also badly detected, because of their having a high red component 
(figure 5). 
The aggregation of the detected sky pixels is made by a simple 
bilinear interpolation on a regular grid, averaging the values from 
different images if they overlap. It leads to artifacts in the envi- 
ronment map: discontinuities are visible between the areas ex- 
tracted from different images, for the reasons mentioned in sec- 
tion 2.2. Furthermore, there are holes in the environment map, for 
the directions where no sky is visible or detected in any image; 
this occurs principally for the areas close to the horizon. We limit 
the extent of these holes by using images taken while the vehicle 
goes through a crossroads, so we have a maximum solid angle of 
visible sky. Then, an interpolation is performed to fill the holes. 
This interpolation leads to more artifacts in the areas with no sky 
pixels extracted (figure 8). The discontinuities can be reduced by 
image processing techniques of blending, for instance by solv- 
ing a Poisson equation, using only reliable pixels in the data term 
(Bhat et al., 2008). However, the discontinuities mainly affect 
the visual quality, and are not a problem in themselves for the 
light simulation. The problem is to retrieve an environment map 
with values closest as possible to the sky radiance at the time of 
acquisition. 
3.2) Estimation of a parametric model 
Another possible approach is to use a parametric model to re- 
construct the environment map. The most widely used model is 
the Perez model (Perez et al., 1993), that uses 5 parameters a, b, 
c, d, e to describe the fall-off of the light around the sun posi- 
tion, plus 1 parameter L to set the zenithal radiance. However, 
this model is limited to the description of low spatial frequency 
phenomena, and therefore cannot model the clouds. The detec- 
tion now avoids the clouds and extract only the background blue 
sky pixels, by using hue and saturation thresholds proposed by 
(Schmitt and Priese, 2009): 
190° < hue < 240° and saturation > 0.2 (2) 
The overexposed pixels, detected before the flat-field correction, 
are rejected. The parameters estimation is then performed by 
non-linear least square fitting, and gives coherent results as long 
as the sky pixels extracted are scattered homogeneously in the 
hemisphere. However, this estimation is affected by the radio- 
metric effects mentioned in 2.2. Predominantly, the bloom effect 
in the images for which the sun is close to their field of view, 
leads to an overestimation of the values of the estimated Perez 
model (figure 8). 
   
    
       
  
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