edge effects in propagation tests

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www.issw2013.com www.issw2013.com Edge effects in propagation tests Edward (Ned) H. Bair 1,2* , Ron Simenhois 3 , Alec van Herwijnen 4 , and Karl Birkeland 5 1 US Army Corps of Engineers Cold Regions Research and Engineering Laboratory, Hanover, NH, USA 2 Earth Research Institute, University of California, Santa Barbara, CA, USA 3 Southeast Alaska Avalanche Center, Juneau, AK, USA 4 WSL Institute for Snow and Avalanche Research SLF, Davos, Switzerland [email protected]

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Edge effects in propagation tests Edward (Ned) H. Bair 1,2* , Ron Simenhois 3 , Alec van Herwijnen 4 , and Karl Birkeland 5 1 US Army Corps of Engineers Cold Regions Research and Engineering Laboratory, Hanover, NH, USA - PowerPoint PPT Presentation

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Page 1: Edge effects in propagation tests

www.issw2013.comwww.issw2013.com

Edge effects in propagation tests

Edward (Ned) H. Bair1,2*, Ron Simenhois3, Alec van Herwijnen4, and Karl Birkeland5

 

1 US Army Corps of Engineers Cold Regions Research and Engineering Laboratory, Hanover, NH, USA2 Earth Research Institute, University of California, Santa Barbara, CA, USA3 Southeast Alaska Avalanche Center, Juneau, AK, USA4 WSL Institute for Snow and Avalanche Research SLF, Davos, Switzerland5 US Forest Service National Avalanche Center, Bozeman, MT, USA

[email protected]

Page 2: Edge effects in propagation tests

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Introduction, propagation test length guidelinesExtended Column Test (ECT), l = 90 cm

Propagation Saw Test (PST),l = 100 cm or slab depth; whichever is greater

Greene, E., et al., 2010: Snow, Weather, and Avalanches: Observational Guidelines for Avalanche Programs in the United States, 136.

Page 3: Edge effects in propagation tests

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Introduction, stress concentration at edges

Page 4: Edge effects in propagation tests

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• G – energy release rate of the slab• G∞ – asymptotic energy release rate (no far

edge effect)• F(r/l) – correction factor• r is crack length• l is test length

G and G∞

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Page 5: Edge effects in propagation tests

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• 163 PSTs and ECTs on beams with l = 1-10 m, including some centered ECTs and PSTs

• Particle tracking on markers inserted into beams

• Finite element modeling for 3 profiles from pits done at tests

Overview

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Page 6: Edge effects in propagation tests

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1. Full crack propagation decreased with test length

2. Greater collapse occurred at the trigger and far end of the beam than in the center

3. Wavelengths were ~ 3 m, 2x what is predicted by the anticrack model

4. The far edge effect is significant for tests up to ~ 2 m

Major findings for ECTs and PSTs

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Page 7: Edge effects in propagation tests

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Field test summary

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Page 8: Edge effects in propagation tests

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• Relative to the middle of the beam, the trigger edge collapsed 160% and the far edge collapsed 128%.

Particle tracking, collapse amplitude

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Page 9: Edge effects in propagation tests

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Particle tracking, wavelength

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Page 10: Edge effects in propagation tests

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FE profiles

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Page 11: Edge effects in propagation tests

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• 3 profiles (a,b,c)• fixed crack length

(critical length) for each profile

Finite element (FE) results

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Page 12: Edge effects in propagation tests

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Correction factor from FE

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Page 13: Edge effects in propagation tests

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• We experimented with centered PSTs (CPSTs) and found that the critical length doubled.

• CPSTs require 2x as much digging for the same crack propagation length as a standard PST, so we find them less practical.

Centered tests

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Page 14: Edge effects in propagation tests

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• We were able to track the collapse amplitude over time for some of the tests that failed on the same layer.

• The average decrease was 0.65 mm/day.

Cool aside

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Page 15: Edge effects in propagation tests

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• PST and ECT results are sensitive to test length• Longer tests could decrease false unstable results,

*BUT* we need to test this hypothesis.• To test our hypothesis, we will examine the

accuracy of 2 m tests vs. standard 1 m tests on slope stability.

Implications

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