2000
DOI: 10.1016/s1464-1909(00)00098-8
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Numerical simulation of real debris-flow events

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Cited by 57 publications
(31 citation statements)
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“…The model satisfactorily captures height and shape of the waves, but it underestimates their duration, overestimating as a consequence, their number. Results are, however, encouraging and comparable with those obtained by Fraccarollo and Papa [16] and Zanuttigh and Lamberti [18].…”
Section: Non-cylindrical Rectangular Channel Test This Test Case Prosupporting
confidence: 59%
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“…The model satisfactorily captures height and shape of the waves, but it underestimates their duration, overestimating as a consequence, their number. Results are, however, encouraging and comparable with those obtained by Fraccarollo and Papa [16] and Zanuttigh and Lamberti [18].…”
Section: Non-cylindrical Rectangular Channel Test This Test Case Prosupporting
confidence: 59%
“…The rheological model adopted for simulations is the Herschel-Bulkley model (eqn (48)). Referring to the simulations carried out by Fraccarollo and Papa [16] on the same event, K is assumed to be 150 Pa路s 1/3 , t c is equal to 925 N/m 2 , and h has been empirically set equal to 1/3.…”
Section: Non-cylindrical Rectangular Channel Test This Test Case Promentioning
confidence: 99%
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“…2 D empirical models like LAHARZ [29], DFLOWZ [5], TopRunDF [49] or TopFLowDF [50] provide a quick view on potential endangered areas and have been applied for several hazard analyses [17,21,40,45,54]. More complex simulation models in engineering practice are based on an "equivalent fluid" approach [25], routing such mass flows in one or two dimensions along the talweg or over a digital elevation model solving depth averaged flow equations [11,16,26,35,36,39]. Such models, like DAN3D [25], Flo2D [39], RAMMS [11] or SAMOS [47], are physically based and consider the momentum or energy conservation of the flow.…”
Section: Introductionmentioning
confidence: 99%
“…Many researchers have developed rheological models for mudflows and debris flows. Theses models can be classified as: Newtonian models (Johnson, 1970;Trunk et al, 1986;Hunt, 1994;Hungr, 1995;Rickenmann, 1999), Bingham model (Johnson, 1970;O'Brien and Julien, 1988;Liu and Mei, 1989;Jan, 1997;Whipple, 1997;Fraccarollo and Papa, 2000;Pastor et al, 2004), Herschel-Bulkley model Garc铆a, 1997, 1998;Imran et al, 2001;Rema卯tre et al, 2005;Rickenmann et al, 2006), generalized viscoplastic model (Chen, 1988), dilatant fluid models (Bagnold, 1954;Takahashi, 1978Takahashi, , 1991Mainali and Rajaratnam, 1994), dispersive or turbulent stress models (Arai and Takahashi, 1986;O'Brien and Julien, 1988;Hunt, 1994), biviscous modified Bingham model (Dent and Lang, 1983), and frictional models (Iverson, 1997;Chen and Lee, 1999;Arattano and Franzi, 2003;Pastor et al, 2004;Rickenmann et al, 2006;Naef et al, 2006). Takahashi and Tsujimoto (1984) presented a twodimensional finite difference model for debris flows based on a dilatant-fluid model coupled with coulomb flow resistance, and modified the model to include turbulence (Taka-hashi et al, 1991(Taka-hashi et al, , 1992.…”
Section: Introductionmentioning
confidence: 99%