Numerical Simulation of Tsunami Propagations and Run-up

Author(s):  
Chiaki Goto ◽  
Nobuo Shuto
Keyword(s):  
2015 ◽  
Vol 70 (9) ◽  
pp. 2270-2281 ◽  
Author(s):  
Asghar Farhadi ◽  
Homayoun Emdad ◽  
Ebrahim Goshtasbi Rad

2012 ◽  
Vol 24 (6) ◽  
pp. 899-913 ◽  
Author(s):  
Wen-Shuo Tsung ◽  
Shih-Chun Hsiao ◽  
Ting-Chieh Lin

2018 ◽  
Author(s):  
José Manuel González-Vida ◽  
Jorge Macías ◽  
Manuel Jesús Castro ◽  
Carlos Sánchez-Linares ◽  
Marc de la Asunción ◽  
...  

Abstract. The 1958 Lituya Bay landslide-generated mega-tsunami is simulated using the Landslide-HySEA model, a recently developed finite volume Savage-Hutter Shallow Water coupled numerical model. Two factors are crucial if the main objective of the numerical simulation is to reproduce the maximal run-up, with an accurate simulation of the inundated area and a precise re-creation of the known trimline of the 1958 mega-tsunami of Lituya Bay. First, the accurate reconstruction of the initial slide. Then, the choice of a suitable coupled landslide-fluid model able to reproduce how the energy released by the landslide is transmitted to the water and then propagated. Given the numerical model, the choice of parameters appears to be a point of major importance, this leads us to perform a sensitivity analysis. Based on public domain topo-bathymetric data, and on information extracted from the work of Miller (1960), an approximation of Gilbert Inlet topo-bathymetry was set up and used for the numerical simulation of the mega-event. Once optimal model parameters were set, comparisons with observational data were performed in order to validate the numerical results. In the present work, we demonstrate that a shallow water type of model is able to accurately reproduce such an extreme event as the Lituya Bay mega-tsunami. The resulting numerical simulation is one of the first successful attempts (if not the first) at numerically reproducing in detail the main features of this event in a realistic 3D basin geometry, where no smoothing or other stabilizing factors in the bathymetric data are applied.


2014 ◽  
Vol 84 ◽  
pp. 38-55 ◽  
Author(s):  
Taemin Ha ◽  
Jaeseol Shim ◽  
Pengzhi Lin ◽  
Yong-Sik Cho

2013 ◽  
Vol 13 (6) ◽  
pp. 393-399
Author(s):  
Wooyoung Jung ◽  
Taekwon Wang ◽  
Yong-Sik Cho

Author(s):  
Maryam Ziaadini-Dashtekhaki ◽  
Mahnaz Ghaeini-Hessaroeyeh ◽  
Saleh Hamzehei-Javaran

Author(s):  
Kyung-Jung Cha ◽  
◽  
Jae-Hwan Jung ◽  
Kwang-Cheol Seo ◽  
Bon-Guk Koo

2013 ◽  
Vol 405-408 ◽  
pp. 1463-1471 ◽  
Author(s):  
Xing Ye Ni ◽  
Wei Bin Feng

To obtain a more detailed description of wave overtopping, a 2-D numerical wave tank is presented based on an open-source SPH platform named DualSPHysics, using a source generation and absorption technology suited for SPH methods with analytical relaxation approach. Numerical simulation of regular wave run-up and overtopping on typical sloping dikes is carried out and satisfactory agreements are shown between numerical results and experimental data. Another overtopping simulation of regular wave is conducted against six different types of seawalls (vertical wall, curved wall, recurved wall, 1:3 slope with smooth face, 1:1.5 slope with smooth face and 1:1.5 slope with stepped-face), which represents the details of various breaking waves interacting with different seawalls, and the average deviation of wave overtopping rate is 6.8%.


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