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Snow avalanche runout from two Canadian mountain ranges

Published online by Cambridge University Press:  20 January 2017

D.J. Nixon
Affiliation:
Department of Civil Engineering, University of British Columbia, Vancouver, B.C., Canada V6T 1z4
D. M. Mcclung
Affiliation:
Department of Civil Engineering, University of British Columbia, Vancouver, B.C., Canada V6T 1z4
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Abstract

Field measurements on maximum runout from two different mountain ranges in Canada are presented and compared: the Coast Mountains in British Columbia and the Rocky Mountains. We include a statistical analysis of topographic terrain parameters such as starting zone catchment area, horizontal reach, vertical drop and relevant slope angles. Following McClung and Mears (1991), we derived a dimensionless parameter which is a measure of runout for each avalanche and we found that the runout ratios (defined below) for a given mountain range obey a Gumbel distribution consistent with previous results. In addition, we found that the runout ratios for both mountain ranges have a length-scale dependence which is potentially very important for land-use planning procedures: the mean value of the runout ratio decreases significantly as the horizontal reach increases. Together with data from other mountain ranges, our results show that path length effects will have to be incorporated when using statistical prediction methods for engineering zoning purposes.

The runout ratio is defined as the quotient of two lengths, Δx/Xβ, where Δ is the horizontal distance from the 10° point to the maximum runout position, and Xβ is the horizontal distance from the start position to the point where slope angle first declines to 10°.

Information

Type
Research Article
Copyright
Copyright © International Glaciological Society 1993
Figure 0

Fig. 1.Definition of geometry and angles to determine extreme runout.

Figure 1

Table 1Descriptive statistics for the Canadian Rocky Mountains and the Coast Mountains of British Columbia

Figure 2

Table 2Multiple regression statistics. Se is the standard error of estimate; R2 is the coefficient of determination

Figure 3

Table 3Location (u) and scale (b) parameters

Figure 4

Fig. 2.Data from the Rocky Mountains and Coast Mountains of British Columbia censored at p = e−1. * denotes Coast Mountains; □ denotes Rocky Mountains.

Figure 5

Table 4Runout ratios for non-exceedance probabilities

Figure 6

Fig. 3Data from the Canadian Rocky Mountains partitioned at Xβ = 1500 m. The three lines represent three values of the non-exceedance probability (― ― ―,p = 0.99), (— — —,p = 0.90), (.....,P = 0.80).

Figure 7

Table 5Comparison of runout distances (Δx ) for seven avalanche paths selected at random from the Rocky Mountains for the regression model αp = −0.784 + 0.956. β� and for the runout ratio model Xp = 0.07 + 0.076(−ln[−ln p])

Figure 8

Fig. 4Comparison of runout predictions for the Rocky Mountains for the least squares (equ.2) and Gumbel distribution (see Table 3) at p = 0.5.