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Fig. 4 shows the results of the experiments performed
during the last two winters (1994-95 and 95-96) in soft
snow (partly new snow/decomposing par ticles/
rounded grains; hand hardness index: fist or 4 fingers).
The mean normal forces for standing atop, weighting
and fifth jump are given together with calculated values
for a static line load (500 N/m) on a homogeneous one
layer snow cover (Schweizer, 1993). The dynamic load
step weighting seems best to correspond to the calcu-
lated static load, whereas standing atop and fifth jump
are smaller and greater respectively.
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The skier stability index has to be supplemented with slab
properties (sublayering). Toinclude ski penetration as pro-
posed by Jamieson and Johnston (1995) is a first step to-
wards an improved skier stability index.
For certain snow conditions the measured skier's im-
pact is of the same order of magnitude as the strength of
weak layer obtained by shear framemeasurements, found
to be typically 500 to 1000 Pa (Föhn, 1993). The dynamic
loads are applied within fractions of seconds (0.03 to 0.3
s). Comparing our field measurements to laboratory test
results (e.g. Narita, 1980) it seems most likely that a skier
will cause (dependingon snow conditions and slab depth)
a deformation in a potential weak layer that is both, large
and fast enough to start brittle failure.
Fig. 5 shows that theimpact increases strongly, but non-
linearly with rutschblock load steps. The substantial in-
crease from step to step is reasonable since it gives the
test more sensibility in the lower stability ranges. The dif-
ferences arising from different snow cover layering and
different weak layers depths explain much of the varia-
tion observed with stability tests and support the sugges-
tions that the rather rough rutschblock scale is by far good
enough and that the rutschblock score alone as a stability
test result far from complete. As important is additional
information on the depth, age and type of weak layer, on
the type of release of the block (whole block or only a part
of it) and on the snow cover (slab) characteristics at the
test site. Only while considering all these information an
extrapolation should be tried.

REFERENCES

Camponovo. C. 1995. (unpublished). Measurements of the ski-
er's impact in the snow cover. Diploma thesis, Eidgenössische
Technische Hochschule, Zürich, Switzerland, 135 pp.

Föhn, P.M.B. 1987. The stability index and various triggering
mechanism. IAHS Publication, 162, 195-214.

Föhn, P.M.B. 1993. Characteristics of weak snow layers or in-
terfaces. In: Proc. Int. Snow Science Workshop, Breckenridge,
Colorado, U.S.A., October 4-8, 1992, 160-170.

Jamieson, J.B. and Johnston, C.D. 1995. Monitoring a shear frame
stability index and skier triggered avalanches involving per-
sistent snow-pack weaknesses. In: Proc. Int. Snow Science
Workshop, Snowbird, Utah, U.S.A., October 30 - November 3,
1994, 14-21.

Narita, H. 1980. Mechanical behavior and structure of snow
under uniaxial tensile stress. Journal of Glaciology, 26 (94), 275-
282.

Schweizer, J. 1993. The influence of the layered character of
the snow cover on the triggering of slab avalanches. Annals of
Glaciology, 18, 193-198.

Schweizer, J., Schneebeli, M., Fierz, C. and Föhn, P.M.B. 1995a.
Field experiments on the dynamic response of the snow cover.
Surveys in Geophysics, 16, 621-633.

Schweizer, J., Camponovo, C., Fierz, C. and Föhn, P.M.B. 1995b.
Skier triggered slab avalanche release - some practical implica-
tions. In: Proc. Int. Symposium: Sciences and mountain - The
contribution of scientific research to snow, ice and avalanche
safety, ANENA, Chamonix, May 30 - June 3, 1995, 309-315.
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static normal force for a line load (500 N/m). Assuming normal and
uniform loading of theload cell (area 0.25 m 2) the normal stress
would correspond to four times the normal force.

DISCUSSION

The measurements show the importance of the weak layer
depth. The impact substantially decreases with increasing
depth, explainingwhy triggering points are often observed
near rocks or to the marginsof a slope, wheresnow depthis
smaller and additionallythe snow cover weaker in general.
In particular for the load stepsstandingatop andweight-
ing thetype of sublayeringof the snow cover is more impor-
tant, or at least as important, as the weak layer depth. Hard
layers causea bridging effect, which distributes the skier's
impact over a larger area, but less efficient in depth. Ski
penetration is directly relatedto layering (surfacehardness)
and is important as well, because the effective weak layer
depth decreases with increasing ski penetration, thereby
increasingstress. However, the large variety of snow cover
conditions makes it very difficult to derive simple rules.
Measurements done by the ski manufacturing industry
and for biomechanical studies indicate that the dynamic
load of skiing (snowplough and parallel turning) is most
comparable to the impact measured on the snow surface
for the load step weighting. For short turns and fast skiing
the impact is greater and similar to the measured one for
jumping. As shown in Fig. 4 the calculated static load due
to a line load correspond to the measured impact for
weighting and can therefore simulate the impact for ski-
ing, however it does not account for layering.
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