The disclosure of the present patent application relates to breakwater systems, and particularly to a method for damping ocean waves in a coastal area to an extent required for different applications using a plurality of parallel slotted vertical barriers to dissipate water wave energy.
An ocean wave contains energy and is the main cause for beach erosion. Around the world, billions of dollars are spent every year for reducing coastal erosion. There are many solutions used around the world, such as seawalls, groin fields, and offshore breakwaters. Each solution has its own merits and demerits. A seawall helps to protect the coastal property from erosion, but accelerates more loss of beach sand. An offshore breakwater using rubble mounds, as seen in
Wave conditions are site specific. The highest wave in 100 years at one location (e.g., the Arabian Gulf) may be 3.0 m, whereas it can be 8.0 m to 10.0 m for the Bay of Bengal or the Atlantic or Pacific Ocean. The transmission coefficient (which is defined as the ratio of transmitted wave height to incident wave height) allowed for reducing beach erosion may be 0.1 at a place with fine sand on the beach, and it can be 0.3 in another place with very course sand and pebbles. Similarly, for an open sea swimming pool, it is necessary to provide higher wave damping for a children's pool than a pool used by adults. In many cases, it may be necessary to dampen a wave to a certain level so that the transmitted wave induced force acting on an existing marine structure, such as open sea aqua-cultural cages or open sea loading/unloading facilities, will be reduced considerably to increase the life span of such structures. Additionally, for many open sea construction activities in the coastal area, a certain order of wave damping is required for successful and uninterrupted construction activities throughout the year. It is also required to allow some small action of waves always on the beach so that the beach quality is maintained throughout the year by the work of nature
Thus, a method for damping ocean waves in a coastal area solving the aforementioned problems is desired.
The method for damping ocean waves in a coastal area uses a barrier having a plurality of vertical walls positioned parallel to each other, each of the walls defining a plurality of horizontally extending slots. The dimensions of the slots, or overall porosity of the wall, can be varied to provide different levels of damping. Similarly, the number of walls positioned parallel to each other may also be varied to provide different levels of damping. Accordingly, a desired amount of damping may be provided through varying the porosity of the walls and the number of walls.
Selecting a proper barrier may include generating charts or referring to charts that provide wave transmission coefficients for barriers having different numbers of walls and different porosities. The selection process may also consider volume of the different barriers (including comparison to a conventional rubble mound breakwater barrier), an amount of horizontal wave force enacted on the different barriers, and an amount of wave induced moment enacted on the different barriers.
These and other features of the present disclosure will become readily apparent upon further review of the following specification and drawings.
Similar reference characters denote corresponding features consistently throughout the attached drawings.
The method for damping ocean waves in a coastal area uses a barrier having a plurality of vertical walls positioned parallel to one another, each wall defining a plurality of horizontally extending slots. The dimensions of the slots, or overall porosity of the wall, can be varied to provide different levels of damping. Similarly, the number of walls positioned in parallel and the positioning of the horizontal slots in neighboring walls at different heights in zig-zag manner may also be varied to provide different levels of damping. Accordingly, a desired amount of damping may be provided through varying the porosity of the walls and the number of walls. U.S. Pat. No. 9,447,554, issued to Neelamani (one of the present inventors) et al. on Sep. 20, 2016, which is hereby incorporated by reference in its entirety, discloses a similar method and structure, but the structure in the '554 patent included a water-impregnable rear barrier behind the slotted vertical walls so that there is essentially no wave transmitted behind the barrier, and the method was directed towards the problem of waves reflected back from the barrier, being directed towards the interior portions of marinas, ports, and harbors, rather than protection from soil erosion and other problems arising from ocean waves impacting coastal areas.
The method for damping ocean waves in a coastal area may include use of a barrier 10 having a plurality of slotted vertical walls forming a barrier 20a, as shown in
In use, a plurality of the vertically extending walls 22 are provided, where each vertically extending wall 22 has a plurality of horizontally extending slots 24 formed therethrough. The areas and/or configurations of the horizontally extending slots 24 can be varied such that each vertically extending wall 22 has a unique degree of porosity. In the example of
In order to form the vertically extending barrier 20a for damping ocean waves in a coastal area, a user selects one or more vertically extending walls 22. In
The slats 26 of each vertically extending wall 22 dampen the energy of the incoming waves W, and the slots 24 between the slats 26 permit the waves W to pass through the walls 22 with reduced wave energy. Compared to a conventional rubble mound breakwater (shown in
For example, if the water depth in
The optimal number of vertically extending walls 22 forming the barrier 20a or 20b and the degrees of porosity associated therewith can be selected based on a desired Kt value (wave transmission coefficient) and/or a minimum number of walls 22 for obtaining desired wave transmission characteristics, which can be equivalent to or better than conventional, sloped rubble mound breakwaters. Kt can be calculated using the following equation:
Kt=Hts/His
where His is the significant incident wave (wave entering barrier) height and Hts is the significant transmitted wave (wave transmitted through or from the barrier) height. The significant wave height is defined as the average top one-third wave heights in a random wave time series acting on the vertical slotted barrier 20a or 20b. As is known in the art, the Kt value is a function of many parameters, including the number of vertical slotted walls 22, the porosity, the significant wave height, the wavelength corresponding to the peak wave period, and the water depth. The relative water depth is calculated as:
d/Lp
where d is a depth of water in the coastal area at the structure location and Lp is an incident wavelength of the water wave W in the coastal area corresponding to peak wave period, Tp. The relative significant wave height is calculated as:
His/d.
Once the number of vertically extending walls 22 and the desired porosity of the walls 22 have been selected, the barrier 20a or 20b is positioned in the coastal area transverse to the direction of the ocean waves for dissipation of water wave energy (i.e., providing an offshore breakwater in the desired region).
Physical models of the barriers were tested using a wave flume at the Kuwait Institute for Scientific Research, Kuwait. The amount of porosity was varied on the models, which included 5% and 10% to 60% with increments of 10%. Additionally, each porosity variant was tested with 1 to 6 walls 22. Random waves of a wide range of significant wave height and peak periods were tested on each model. The tested relative significant wave heights include 0.071, 0.142, and 0.214. Each relative significant wave height was tested with relative water depths of 0.1 to 0.5 at increments of 0.1.
The transmitted wave time series was measured for the input conditions. Additionally, wave forces and moments were also recorded to provide information pertaining to stability and chance of overturning of the slotted wave barrier structure. Models of conventional, rubble mound breakwaters were also tested. The conventional, rubble mound breakwaters were tested at three heights: submerged crest, crest and still water at same level, and emerged crest level. A crest of the submerged rubble mound was set at approximately 85% of the water level, a crest of the rubble was set at the water level, and a crest of the emerged mound was approximately 115% the water level. Finally, a single wall with 0% porosity was tested.
Table 1 below lists the different barrier configurations tested and their volume in relation to the conventional rubble breakwaters. In column 3, n indicates the number of walls 2222 and P indicates the porosity percentage provided by the slots 24. The rightmost column indicates a percentage of material volume used for the slotted wall (V1) versus an emerged, conventional rubble breakwater (V2).
For example, as seen in Table 1 above, a slotted barrier having 1 wall with 10% porosity has 0.84% the volume of an emerged, rubble breakwater. The highest volume percentage compared to the emerged, rubble breakwater is 5.34% for the slotted barrier with six walls having 5% porosity.
Table 2 below provides an example of a table that may be used for selecting a proper slotted barrier based on relative water depth (d/Lp), relative significant wave height (His/d), and wave transmission coefficient (Kt). Lp is the wavelength that corresponds to the peak period. Table 2 indicates which (n,P) combinations from Table 1 resulted in 0.1<KT<0.15 for multiple relative water depths and significant wave heights.
Table 2 will facilitate a user in selecting the proper slotted vertical barrier if the user knows the relative water depth and relative significant wave height of the location requiring wave damping, as well as a desired Kt value (0.1<Kt<0.15). Similar charts can be created (and are available from the inventors) for different relative water depth, relative significant wave height, and Kt values (such as Kt<0.065; 0.065<Kt<0.1; 0.15<Kt<0.2; 0.2<Kt<0.25; 0.25<Kt<0.3; 0.3<Kt<0.35; 0.35<Kt<0.4; 0.4<Kt<0.45; 0.45<Kt<0.5). In addition, Table 1 can be used to further narrow the results of Table 2 based on the amount of material available, or desired, for the breakwater.
Table 3 provides insight into selecting the best performing or most economic slotted vertical barrier, and how the Kt of best performing and most economic slotted vertical barriers compares to the Kt of an emerged, rubble mound breakwater.
The second and third columns indicated relative significant wave height (His/d) and relative water depth (d/Lp) in the ranges of 0.071-0.214 and 0.1-0.5, respectively. The fourth column indicates KtRM, which is the Kt of an emerged offshore rubble mound breakwater structure. The fifth and sixth columns indicate which slotted vertical barriers perform the best based on lowest Kt, and the respective Kt, which is listed as Ktb. The seventh and eight columns indicate which slotted vertical barriers are the most economical and the respective Kt, which is listed as Kte. Most economical is determined by selecting the slotted vertical barrier that has a lower Kt than KtRM with the lowest volume based on the (V1/V2) values in Table 1. The ninth column indicates the number of slotted barrier configurations better than an emerged offshore rubble mound breakwater available among the forty-two slotted vertical barriers tested, as listed in Table 1 (except three different rubble mound breakwater arrangements and one vertical wall structure with 0% porosity). The tenth column indicates the percentage of improvement over KtRM for the best performing slotted vertical barrier, and the eleventh column indicates the percentage of improvement over KtRM for the most economical barrier. As seen above, even the most economical barrier has a significant improvement over the rubble mound breakwater.
Fn=FXS/0.5*ρ*g*His*d*W
where FXS is the significant horizontal wave force in newtons, ρ is the mass density of water (1000 kg/m3), g is the acceleration due to gravity (9.81 m/s2), His is the significant incident wave height in meters, and W is the width of the barrier in meters. The x-axis indicates the configuration number front Table 1. As seen in the drawing, the normalized wave force exerted on the slotted vertical barriers decreases with an increase in porosity. Therefore, a desired transmission coefficient Kt and normalized wave force Fn can be achieved by increasing the porosity to decrease the normalized wave force Fn and increasing the number of walls 22 to maintain the desired transmission coefficient Kt. Accordingly, normalized horizontal force Fn may be used for the design of the slotted vertical barrier against horizontal sliding.
Mn=Mys/0.5*p*g*His*d*W,
where Mys can be estimated using the following equation:
Mys,=0.6145*d*FXS
and the remaining variables are the same as discussed above. The wave-induced moment is equal to the product of the total horizontal wave force and the lever arm from the base. The estimation of the significant moment Mys based on the horizontal wave force FXS is good with a correlation coefficient R2 of 0.9485. The wave induced moment can be used to check the stability of the slotted wave barrier structure against overturning.
It is necessary to consider the wave-induced moment exerted on the barrier when determining if the waves will cause the barrier to overturn. Since the normalized wave induced moment Mn is directly correlated to the normalized horizontal force Fn, an increase in porosity results in a decrease in wave induced moment Mn. Therefore, a desired transmission coefficient Kt and wave induced moment Mn can be achieved by increasing the porosity to decrease the wave induced moment Mn and increasing the number of walls 22 to maintain the desired transmission coefficient Kt. Additionally, the size and weight of the horizontal support plate 28 at the bottom of the barrier 20a or 20b may be altered to provide additional stability against sliding and overturning.
It is to be understood that the present method for damping ocean waves in a coastal area is not limited to the specific embodiments described above, but encompasses any and all embodiments within the scope of the generic language of the following claims enabled by the embodiments described herein, or otherwise shown in the drawings or described above in terms sufficient to enable one of ordinary skill in the art to make and use the claimed subject matter.
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