|
Dept. of Civil Engineering, University of Calgary, 2500 University Dr. NW

Calgary AB T2N 1N4, Canada. fax: 1 403 282 7026, e-mail: jschweiz@acs.ucalgary.ca
|
 |
|
Keywords: snow mechanics, snowstrength, snow tempera-
ture, snow failure, fracture

ABSTRACT.

Snow samples (115 mm in diameter, 16-18 mm in height)
were taken from the field and shortly afterwards tested in
a cold laboratory using a direct simple shear apparatus of
Norwegian manufacture. The effectsof strain rate andtem-
perature on snow strength, stiffness and toughness were
studied. The transition from ductile to brittle behaviour
was found to be at a strain rate between10-4 and 10-3 s-1 for
the snow types and temperatures tested. Stiffness up to
peak stress proved to be highly temperature dependent.
Toughness is also significantly temperature dependent,
while snow strengthseems to dependonly slightly on tem-
perature. The dependence of the shear strength on
temperatureseems partly hidden by the scatter in strength
data due to variations inherent in sampling and testing.

INTRODUCTION

The behaviour of snow under shear is believed to be one of
the most important factors for describing slab avalanche
formation and assessing the snow stability. Although most
previous controlled shear experiments were done using
slow displacement rates, fieldtests of snow strength or slab
stability such as the rutschblock test involve rapid but less
controlledloadingandstrainrates. Previoustestingin shear
under laboratory conditions was done by Ballard et al.
(1965), McClung (1977) and Fukuzawa(1993). Some field
studies: Roch (1966), Perla (1977), Föhn (1987) and
Jamieson (1995). Recently Föhn and Camponovo (1996)
have tried to measure shear strength in situ under
controlled conditions.

METHODS

Testswere performed with a Norwegiantype directsimple
shear apparatus in the cold laboratory at Rogers Pass, Gla-
cier National Park (British Columbia, Canada) (Fig. 1). The
effects of shearing rate and temperature were studied. In
particular,to establish the ductileto brittle transition, rapid
tests at strain rate larger than 10-4 s-1 were performed.
Specimens (115 mm in diameter, 16-18 mm in height)
were taken from relatively homogeneous layers of fine
grained snow with densities between 220 and 340 kg/m3 ,
and handhardness index: 3 (1 finger) to 4 (pencil). These
were tested at -5, -10 and -15 ºC for six different displace-
ment rates: about 0.0073 mm/min, 0.074 mm/min, 0.17
mm/min, 0.29 mm/min, 0.50 mm/min, and 4.2 mm/min.
For eachof the displacement rates andtemperatures about
5 tests were performed, resultingin a total of about 90 tests.
Typically, samples were tested at a certain displacement
rate on three consecutive days at the three temperatures.
Accordingly, samples were stored typically between 1 and
5 days. This procedure may have slightly affected the
results due to ongoing age-hardening.
|
|
 |
|
The normal force applied was 4.9 N, which corresponds
to a stress of 470 Pa, and was kept constant during all
experiments. During the tests horizontal and vertical
displacements, and the applied horizontal (shear) force
were measured and recorded. Due to hard-/software limi-
tations the maximum possible scan frequency was only
10 Hz, which proved to be insufficient for the most rapid
displacement rates (strain rates between 10-3 and 10-2 s-1 ),
so the number of measurements is generally too small to
establish a reliable stress-strain curve.
The shear strength (failure or peak stress) is defined as
the maximum stress, the peak, on the stress-strain curve.
The initial slope of the stress-strain curve is called stiff-
ness, and represents initial resistance to shear deforma-
tion. Stiffness as given below is the slope of the secant
intersectingthe stress-straincurve at80%of the peakstress.
Strain rates, calculated from the time-displacement (or
strain) curve, are typically not constant during the tests,
since horizontaldisplacement(andaccordinglystrain)does
not increase linearly with time. The strain rates given in
the following sections are mean values calculatedfrom the
deformation at failure, the time to failure and the sample
thickness.

Effect of strain rate

Typical stress strain-curves for three different strain rates
are shown in Fig. 2. Curve (a) shows the response of the
stressed snow sample for a strain rate of 6.1 = 10-5 s-1 ; test
duration was 80 min. The curve shows typical strain sof-
tening behaviour with a ductile type of failure character-
ized by large deformation and high toughness or energy
absorption capability as evidenced by the area under the
stress-strain curve. Curve (b) is typical for the tests per-
formed with strain rates of about 10-4 s-1 and is believed to
|
 |