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Figure 1. (A) Subset of NAC image M135433752LE covering a
boulder field situated around -30.4°lat and 322.5°lon
(B) Groups of pixels detected as bright faces of boulders on the
image (colors correspond to ranges of size)
2.5 Risk Maps
The computation of risk maps for one specified landing area is
mainly based on three hazards: slope, roughness and shadow.
Slope and roughness hazard maps are computed from the high
resolution DTM while the shadow map is produced by the
illumination module (s. next section). The risk map
computation consists of the combination of all hazards in one
binary (safe/unsafe) landing risk map at a certain alpha-level.
The alpha level is the probability that the threshold is
outmatched (toward infinite) using a normal probability
distribution function centered on the current value and with a
dispersion defined by the error map (variance). Each hazard
map is transformed into a binary risk-score map at a certain
alpha-level according to user-defined thresholds. The error on
the hazard is taken into account in the comparison between the
current value of the hazard and the threshold. The final landing
risk map is computed by multiplication of individual risk score
maps and taking into account the landing position uncertainty
(Bonfiglio et al. 2011).
2.6 Illumination Maps
Before being able to generate any illumination product for a
target area, the illumination module generates a horizon mask
using a ray-tracing algorithm. On the basis of a DTM it
computes in each pixel of the target area and for each direction
the biggest elevation angle of an obstacle along this direction.
Using the horizon mask corresponding to a specified time (i.e. a
specified sun direction), an instantaneous illumination map
showing the proportion of the solar disk visible in each pixel
and an incoming flux map providing the irradiance in Watt/m?
at a specified time can be computed.
Maps characterizing the illumination conditions on a certain
period can also be produced like the accumulated Sun
illumination fraction map (providing for each pixel the Sun
illumination fraction for a period of analysis), the longest quasi
continuous illumination period (LQCIP) or the longest period of
darkness (LPOD), and others (Vanoutryve et al. 2010).
2.7 Temperature Maps
This module can be subdivided into two parts. The first one
allows the generation and update of one pre-processed set of
3D-grid data containing an aggregation of all brightness
temperature measurements from LRO DLRE (Paige et al. 2010)
in three thermal channels (7, 8 and 9) of the instrument since
the beginning of the observations. These three brightness
temperature values provided in DLRE RDR tables in the NASA
PDS supply the 3D-grid established with a predefined time step
and spatial resolution for a typical lunar day on the whole moon
surface, excluding the effect of eclipses and other incoherent
data (filtered using quality flags). A temporal filter is applied to
smooth erratic values and linear interpolation is computed for
the spatiotemporal pixels where no DLRE brightness
temperature data is directly available. Surface temperature is
considered equivalent to brightness temperature because the
moon soil emissivity in the wavelengths of the three channels is
considered equal to 1. This condition is verified by the high
correlation between the different channels (Paige et al. 2010).
The second part of the temperature module allows the
generation of two kinds of surface temperature products from
this dataset. A low resolution temperature map can be obtained
for one specified time (interpolated from the dataset described
above) and the mean diurnal variation of the surface
temperature at one specified point can be plotted in a diagram.
2.8 Reflectance Maps
Reflectance maps are computed from LROC NAC or WAC
(Wide-Angle Camera) radiance images. The reflectance can be
understood as the ratio (value between 0 and 1) between the
power re-emitted by the surface (in all directions of the
hemisphere above the observed target) and the received flux
from the Sun on this surface (7 the irradiance). It does not
depend on the topography, nor on the illumination conditions; it
only depends on the physical characteristics of the surface.
Sun position, sensor position and surface topography must be
known to compute reflectance from a set of radiance images.
Several reflectance models can be used to estimate the
reflectance from radiance images (Lambertian, Lunar-Lambert
and Hapke models are forescen for LandSAfe).
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