2002
DOI: 10.5194/nhess-2-187-2002
|View full text |Cite
|
Sign up to set email alerts
|

Experimental investigation on steady granular flows interacting with an obstacle down an inclined channel: study of the dead zone upstream from the obstacle. Application to interaction between dense snow avalanches and defence structures

Abstract: Abstract. An experimental investigation with dry granular flows passing over an obstacle down a rough inclined channel has been performed. The aim is to improve our understanding of the interaction between dense snow avalanches and defence structures. Specific attention was directed to the study of the zone of influence upstream from the obstacle, linked to the formation of a dead zone. The dead zone length L was systematically measured as a function of the obstacle height H and the channel inclination θ , for… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

2
13
0

Year Published

2003
2003
2021
2021

Publication Types

Select...
7
1

Relationship

0
8

Authors

Journals

citations
Cited by 41 publications
(15 citation statements)
references
References 7 publications
2
13
0
Order By: Relevance
“…Figure 6d shows that for increasing Fr, the standoff distance decreases dramatically from a maximum of ∼2.0 m in the range of Fr < 5, and then levels out at around 1 m for Fr > 5. This result agrees qualitatively with the findings of Cui and Gray (2013) and Faug et al (2002) on the standoff distance of granular bow shocks and size of mobilized domains, respectively. Interestingly, a similar dependency is found experimentally between the drag coefficient of a wall and Fr in a mud flow by Tiberghien et al (2007), as well as for the hydrodynamic impact pressure of debris flows and Fr by Proske et al (2011).…”
Section: Microscale Processes Of Impact Pressure Buildupsupporting
confidence: 91%
“…Figure 6d shows that for increasing Fr, the standoff distance decreases dramatically from a maximum of ∼2.0 m in the range of Fr < 5, and then levels out at around 1 m for Fr > 5. This result agrees qualitatively with the findings of Cui and Gray (2013) and Faug et al (2002) on the standoff distance of granular bow shocks and size of mobilized domains, respectively. Interestingly, a similar dependency is found experimentally between the drag coefficient of a wall and Fr in a mud flow by Tiberghien et al (2007), as well as for the hydrodynamic impact pressure of debris flows and Fr by Proske et al (2011).…”
Section: Microscale Processes Of Impact Pressure Buildupsupporting
confidence: 91%
“…At time t = 0•19 s ( Fig. 4(b)), sand begins to deposit, forming a dead zone (Faug et al, 2002;Gray et al, 2003;Ashwood & Hungr, 2016) near the base of the barrier. Subsequent flow impacts the wedge-like dead zone, beginning to run up along the face of the barrier.…”
Section: Interpretation Of Resultsmentioning
confidence: 99%
“…Interaction between dry granular flows and a single obstacle has been investigated, revealing key impact mechanisms, such as dead-zone development (Faug et al, 2002;Gray et al, 2003), runup (Mancarella & Hungr, 2010;Choi et al, 2015) and overflow (Hákonardóttir et al, 2003a(Hákonardóttir et al, , 2003bChoi et al, 2014a). Analytic solutions have also been proposed: for example, Faug (2015a) conducted a series of small-scale experiments using dry sand flow impacting obstacles along an incline.…”
Section: Introductionmentioning
confidence: 99%
“…up by the tail of the flow, flowing at lower speeds than the bulk of the avalanche. An experimental study of these wedges behind catching dams of varying heights and the so-called 'dead zones' behind the dams for lower Froude number flows (2 < Fr < 6) has been carried out by Faug et al (2002). Numerical calculations of the dead zone behind an obstacle of an infinite height are described by Gray et al (2003).…”
Section: Jet Deflectionmentioning
confidence: 99%