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Fig.5: Hard slab stopped by steel bridges, Val Giandains-Pontresina
small slabs have to be prevented as well, the distance
between the lines of structures should be reducedand the
supporting plane should be more dense.
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SAFETY ANALYSIS OF AREAS CONTROLLED WITH

SUPPORTING STRUCTURES

Afterthe building of supporting structures the protective
effect has to be taken into account forthe revision of haz-
ard mapswithrespect toland-use planning.Supporting
structuresreducethe probability of avalanche fractureand
theirextent.Thefollowingquestionsarecrucial:which
degreeofsafetycanbeattained belowcontrolledareas,
how much smaller arethe hazard zones? According to our
experiencethereareno generalsolutions. Every singlecase
has its own characteristics. InSwitzerland theresponsibles
are
verycautiousinreducing hazardzones.Changing a
red zone (high hazard) into a white one (no hazard) after
the
realization ofsupportingstructures isanexception,
often a blue zone (low hazard)is introduced. Todetermine
the
residualriskbelowacontrolledareathefollowing
criterias should be checked:
Extent of the starting zone

Often the terrain of starting zones is very complex.Be-
side orbelow the main starting zone which is control-
led there are secondary ones which are then decisive
foravalanche dynamic calculations.The frequency of
these avalanchesis often smallercompared with those
of the main path.
Arrangement of structures

Thearrangement ofthe structuresshould correspond
to the Swiss Guidelines(1990). Important points are the
upper and lower boundaries of the controlled area, the
slope distance between the lines of structures and the
lengthof the lines. In every starting zonethereareplaces
like narrow gullies or steep rockcliffs that are more dif-
ficult to control. Avalanchesreleasedincontrolledareas
are calculated with reduced flow rates due to smaller
velocities or lower turbulent friction parameter x . Either
the speedis calculatedafter adistancethat corresponds
to the slopeparalleldistancebetweentwo structurelines
orthe turbulent friction parameterxis reduced to 280
m/s2 .
Extreme snow depth
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Fig.6: Snow net andsteel bridges in a springtime situation, Oberalp

According to the Swiss Guidelines (1990) supporting
structures are designed for the 100-year extreme snow
depth expected at the site. However for hazard map-
ping events up to 300 years have to be considered in
Switzerland. Thereis a risk that structures are filled up
before an important snow fall occurs and a slab is
releasedover the structures. At Weissfluhjoch (2540 m
a.s.l.) maximal snow depths are recorded normally be-
tween March and May and the most frequent snowfall
periods are in average between December and Febru-
ary. There are no approved methods yet to determine
realistic fracture depthfor avalanche dynamic calcula-
tions as a function of extreme snow depth and for a
return period T of 300 years. In practice the following
rough estimates could be used:

I. It is assumed that the difference DH between the struc-
ture height H k and the 300 years extreme snow depth
H
meanex t expected in the starting zone corresponds to the
fracture depth. The necessary data originate from
observation series over up to 60 years of the SFISAR
network. With the mean slope y the slab thickness d
can be computed from the snow depth difference DH0
according to Salm et al. (1990).

Example for Weissfluhjoch (2540m):

Hex t =456cm (T~300years)
Hk =411cm (T~100years)
[!]H =456-411=45cm

II. It is assumed that theprobability P
e k that thesnow height
equals the structur height Hk times the probability P
for a certain increase of snow depth within 3 consecu-D
tive days (H3, is equal to 1/300, corresponding to the
probability used in hazard mapping:

Example for Weissfluhjoch (2540m):

Hk =411cm - D(T~100years- Pk =1/100
1/300=1/100 - PD - P
D=1/3(T D=3years
An increase of snow depth within 3 consecutive days
DH3 of 79 cm corresponds to a return period TD of 3
years. This is nearly the double compared to I. Prob-
ably it is overestimated because of less intense snow-
fall during the time of maximum snow depth. Withthe
mean slope y the slab thickness d
0 can be computed
from DH3 according to Salm et al. (1990).
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