scholarly journals ANALYTICAL AND NUMERICAL STUDIES OF OBLIQUE WAVE INCIDENCE ON IMPEDANCE-MATCHED GRADED INTERFACES BETWEEN RHM AND LHM MEDIA

2022 ◽  
Vol 107 ◽  
pp. 131-140
Author(s):  
Brage B. Svendsen ◽  
Balwan Rana ◽  
Mariana Dalarsson
1986 ◽  
Vol 1 (20) ◽  
pp. 100
Author(s):  
M.A. Losada ◽  
A. Sanchez-Archilla ◽  
C. Vidal

A simple model to predict the longshore current velocity at the breaker line on a beach with oblique wave incidence, is presented. The model balances driving and resistance terms (gradients of radiation and turbulent Reynolds stresses and bottom friction) to get a general expression for the velocity. This equation shows explicitely the influence of Iribarren's parameter on longshore current generation. It has been tested with field and laboratory data, obtaining a reasonable fit to measured values. The resulting (predictive) model is expected to be valid for any type of breakers though the calibration has been mainly done for spilling and plunging types, due to the scarcity of results for other breakers.


2012 ◽  
Vol 117 (F3) ◽  
pp. n/a-n/a ◽  
Author(s):  
N. van den Berg ◽  
A. Falqués ◽  
F. Ribas

2011 ◽  
Vol 1 (32) ◽  
pp. 85
Author(s):  
Toshinori Ishikawa ◽  
Takaaki Uda ◽  
Toshiro San-nami ◽  
Shusuke Watanabe

In the Ukishima region of Lake Kasumigaura, beach nourishment along with the construction of groins has been carried out to recover a sandy beach. After the beach nourishment, part of the nourishment sand was transported away from the beach, turning around the tip of the downcoast groin owing to the oblique wave incidence in winter. To enhance the stability of the beach, the groins were extended and a spur dike was constructed. To design these structures, a numerical simulation using the BG model was carried out, and the optimum shapes were determined by taking into account the seasonally changing wave direction. The effectiveness of the spur dike was numerically evaluated using the BG model.


2013 ◽  
Vol 40 (11) ◽  
pp. 2726-2730 ◽  
Author(s):  
R. Garnier ◽  
A. Falqués ◽  
D. Calvete ◽  
J. Thiébot ◽  
F. Ribas
Keyword(s):  

2014 ◽  
Vol 1 (34) ◽  
pp. 68
Author(s):  
Sang-Ho Oh ◽  
Chang-Hwan Ji ◽  
Young Min Oh ◽  
Hee Do Ahn

Author(s):  
Lucia Uguccioni ◽  
Rolf Deigaard ◽  
Jørgen Fredsøe
Keyword(s):  

Author(s):  
Dorthe Petersen ◽  
Rolf Deigaard ◽  
Jørgen Fredsøe ◽  
Nils Drønen

1991 ◽  
Vol 224 ◽  
pp. 625-644 ◽  
Author(s):  
Robert A. Dalrymple ◽  
Miguel A. Losada ◽  
P. A. Martin

The linear theory for water waves impinging obliquely on a vertically sided porous structure is examined. For normal wave incidence, the reflection and transmission from a porous breakwater has been studied many times using eigenfunction expansions in the water region in front of the structure, within the porous medium, and behind the structure in the down-wave water region. For oblique wave incidence, the reflection and transmission coefficients are significantly altered and they are calculated here.Using a plane-wave assumption, which involves neglecting the evanescent eigenmodes that exist near the structure boundaries (to satisfy matching conditions), the problem can be reduced from a matrix problem to one which is analytic. The plane-wave approximation provides an adequate solution for the case where the damping within the structure is not too great.An important parameter in this problem is Γ2= ω2h(s- if)/g, where ω is the wave angular frequency,hthe constant water depth,gthe acceleration due to gravity, andsandfare parameters describing the porous medium. As the friction in the porous medium,f, becomes non-zero, the eigenfunctions differ from those in the fluid regions, largely owing to the change in the modal wavenumbers, which depend on Γ2.For an infinite number of values of ΓF2, there are no eigenfunction expansions in the porous medium, owing to the coalescence of two of the wavenumbers. These cases are shown to result in a non-separable mathematical problem and the appropriate wave modes are determined. As the two wavenumbers approach the critical value of Γ2, it is shown that the wave modes can swap their identity.


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