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Fig. 2. Basic setup of the snow stratigraphy profiler.
passing throughpin holes in thefoil of the Polariod sensor.
Vapor that condenses may freeze the foil to the backplane
of the sensor.

Snow Profiler

The Frequency Modulated Continuous Wave profiling
Radar (FMCW) shown in Fig.2 measures a spectrum of
distances from the ground surface to reflecting layer inter-
faces and the snow surface. Specular reflection of micro-
waves dependson the difference of the index of refraction
between consecutive layers and layer thickness.
Specialsoftware at thebase station (e.g. at theavalanche
forecaster's office) permits on-line graphicpresentation of
time-series of electromagnetic profiles of the snow cover.
The electromagnetic profile looks very similar to a tradi-
tional layer profile. With additional software depth and
settling of new snow layers can be determined with fair
accuracy (5%). Settling speed relates directly to the rate
of increase of strength and viscosity but also to the state of
metamorphism (depth hoar inhibits settling). Other
important parameters that can be determined are: snow
depth, water equivalence of a dry snow cover, significant
layer interfaces, avalanchereleases,releaseheight,dammed
melt water at layer interfaces(in spring occasionallyacting
as weak layers), and surface wetness. Because wet snow
significantly attenuatesmicrowavesat frequenciesused for
the profiler, installations are limited to high mountain
release zones where the snow cover stays essentially dry
duringthewinter season. Themain advantageof thesystem
is the possibility to get most important information from
within or close to potential r elease zones of large
avalanches. In large bowls several radar may be installed
at different representative locations to allow for the
monitoring of aspectdependentloading and partial relea-
ses.

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Specifications:

* Frequency modulated continuous C-band radar

* Triangular modulation 4 to 8Ghz at 40Hz

* Approx. conversion rate in air 2kHz/m.

* Approx. conversion rate in dry snow 2.2 to 2.8 kHz/m
depending on snow density.

* Maximum range in dry snow for snow densities below
400kg/m3 is 8m.
The accuracyof the measurementsdependson the qual-
ity of the microwave reflection at the layer interfaces and
of the snow surface, and for the measurements without
reference reflector, on the accuracy of the snow density
estimates ( a change of density by 100kg/m3 corresponds
to a 7% changeof optical distance). The absolute error for
measurements of the waterequivalence of dry snow
amounts to about 5kg/m 2 or 5mm of water equivalence.
The system consists of two separate parts: the radar is
mounted in a water protected cylindrical container with a
max. outer diameter of 68cm and a heightof approx. 80cm.
In field installations this cylindrical radar-container is
installed in a concrete tube that is buried in the ground.
The upperendof thetube is closedby a mechanicallystable
radome that supports the weight of the snow.
The radar connects with a coaxial RG/U 58 cable (up to
700m) to the field data controller that controls the radar,
recharges batteries, initiates measurements and performs
the necessary computing (Fast Fourier Transform). The
radar interface controller connects to the CR10X by the
SDM-bus.Theradarcontroller (CR10X) transmits frequency
spectra (256 points per measurements)to the base station.
The base station software allows individual analysesof the
spectra andconversion to a bitmap presentation as shown
in Fig. 4/5.
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