Iterative source-range estimation in a sloping-bottom shallow-water waveguide using the generalized array invariant

2017 ◽  
Vol 141 (5) ◽  
pp. 3991-3991
Author(s):  
Chomgun Cho ◽  
Hee-Chun Song ◽  
Paul Hursky ◽  
Sergio Jesus
2008 ◽  
Vol 8 (2) ◽  
pp. 175-185 ◽  
Author(s):  
E. van Groesen ◽  
D. Adytia ◽  

Abstract. In this paper we show that shallow, elongated parts in a sloping bottom toward the coast will act as a waveguide and lead to large enhanced wave amplification for tsunami waves. Since this is even the case for narrow shallow regions, near-coast tsunami waveguiding may contribute to an explanation that tsunami heights and coastal effects as observed in reality show such high variability along the coastline. For accurate simulations, the complicated flow near the waveguide has to be resolved accurately, and grids that are too coarse will greatly underestimate the effects. We will present some results of extensive simulations using shallow water and a linear dispersive Variational Boussinesq model.


1987 ◽  
Vol 10 (3) ◽  
pp. 557-562 ◽  
Author(s):  
Yilmaz Akyildiz

We consider the system of nonlinear differential equations governing shallow water waves over a uniform or sloping bottom. By using the hodograph method we construct solutions, conservation laws, and Böcklund transformations for these equations. We show that these constructions are canonical relative to a symplectic form introduced by Manin.


2018 ◽  
Vol 104 (5-6) ◽  
pp. 915-921 ◽  
Author(s):  
A. V. Aksenov ◽  
S. Yu. Dobrokhotov ◽  
K. P. Druzhkov

2007 ◽  
Vol 37 (10) ◽  
pp. 2429-2445 ◽  
Author(s):  
Frode Hoydalsvik

Abstract The mass transport velocity in shallow-water waves reflected at right angles from an infinite and straight coast is studied theoretically in a Lagrangian reference frame. The waves are weakly nonlinear and monochromatic, and propagate in a homogenous, viscous, and rotating ocean. Unlike the traditional approach where the domain is divided into thin boundary layers and a core region, the uniform solution is obtained here without constraints on the thickness of the bottom wave boundary layer. It is shown that the mass transport velocity is not only sensitive to topography, but depends heavily on the interplay between the vertical length scales. Similarities and differences between the cases of a constant depth, a linearly sloping bottom, and a wavy and linearly sloping bottom are discussed. The mass transport velocity can be divided into two main categories—that induced by waves with a frequency close to the inertial frequency, and that induced by waves with a much larger frequency. For waves significantly affected by rotation to first order, the cross-shore mass transport velocity is very small relative to the alongshore mass transport velocity, and the direction of the mass transport velocity is reversed relative to that in waves of much higher frequencies.


Sign in / Sign up

Export Citation Format

Share Document