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Simulation of obliquely interacting solitary waves with a hard wall by using HAWASSI-VBM and SWASH model
Yuliawati L.a, Subasita N.b, Adytia D.d, Budhi W.S.a
a Department of Mathematics, Institut Teknologi Bandung, Indonesia
b LabMath-Indonesia, Lawangwangi, Bandung, Indonesia
c LabMath-Indonesia, Lawangwangi, Bandung, Indonesia
d Applied Mathematics, University of Twente, Enschede, Netherlands
[vc_row][vc_column][vc_row_inner][vc_column_inner][vc_separator css=”.vc_custom_1624529070653{padding-top: 30px !important;padding-bottom: 30px !important;}”][/vc_column_inner][/vc_row_inner][vc_row_inner layout=”boxed”][vc_column_inner width=”3/4″ css=”.vc_custom_1624695412187{border-right-width: 1px !important;border-right-color: #dddddd !important;border-right-style: solid !important;border-radius: 1px !important;}”][vc_empty_space][megatron_heading title=”Abstract” size=”size-sm” text_align=”text-left”][vc_column_text]© 2016 AIP Publishing LLC.In this paper we discuss the comparison of numerical simulations of solitary waves, reflected from a rigid wall under an angle, using the HAWASSI-VBM (Hamiltonian Wave-Ship-Structure Interaction – Variational Boussinesq Model) and the SWASH (Simulating Waves ’till Shore) model. We reconstruct the experiment of Yeh et al (2011) to investigate the amplification of the Mach stem phenomenon. In the simulation, some solitary waves from the solution of Kadomtsev-Petviashivili (KP) equation with the angle of 30° is chosen as the incident wave. We compare the results of numerical simulation with the laboratory experiment of Yeh et al. Based on this comparison, results of numerical simulation from both wave models show a quite good agreement with the experiment data.[/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”Author keywords” size=”size-sm” text_align=”text-left”][vc_column_text][/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”Indexed keywords” size=”size-sm” text_align=”text-left”][vc_column_text]HAWASSI-VBM,oblique wave,reflection,solitary wave,SWASH[/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”Funding details” size=”size-sm” text_align=”text-left”][vc_column_text][/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”DOI” size=”size-sm” text_align=”text-left”][vc_column_text]https://doi.org/10.1063/1.4940832[/vc_column_text][/vc_column_inner][vc_column_inner width=”1/4″][vc_column_text]Widget Plumx[/vc_column_text][/vc_column_inner][/vc_row_inner][/vc_column][/vc_row][vc_row][vc_column][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][/vc_column][/vc_row]