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JPH0522761B2 - - Google Patents
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JPH0522761B2 - - Google Patents

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Publication number
JPH0522761B2
JPH0522761B2 JP60124591A JP12459185A JPH0522761B2 JP H0522761 B2 JPH0522761 B2 JP H0522761B2 JP 60124591 A JP60124591 A JP 60124591A JP 12459185 A JP12459185 A JP 12459185A JP H0522761 B2 JPH0522761 B2 JP H0522761B2
Authority
JP
Japan
Prior art keywords
wave
bag
diving
bags
water
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP60124591A
Other languages
Japanese (ja)
Other versions
JPS62111006A (en
Inventor
Takeshi Ijima
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
HAZAMAGUMI KK
Original Assignee
HAZAMAGUMI KK
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by HAZAMAGUMI KK filed Critical HAZAMAGUMI KK
Priority to JP60124591A priority Critical patent/JPS62111006A/en
Publication of JPS62111006A publication Critical patent/JPS62111006A/en
Publication of JPH0522761B2 publication Critical patent/JPH0522761B2/ja
Granted legal-status Critical Current

Links

Classifications

    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02ATECHNOLOGIES FOR ADAPTATION TO CLIMATE CHANGE
    • Y02A10/00TECHNOLOGIES FOR ADAPTATION TO CLIMATE CHANGE at coastal zones; at river basins
    • Y02A10/11Hard structures, e.g. dams, dykes or breakwaters

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  • Revetment (AREA)

Description

【発明の詳細な説明】 <産業上の利用分野> 本発明は波のエネルギーを反射及び吸収する消
波装置の改良に関する。本発明者は、この発明出
願前の昭和58年3月4日付で、発明の名称「消
波・発電法」について出願したが本願はその改良
に関するものである。
DETAILED DESCRIPTION OF THE INVENTION <Industrial Application Field> The present invention relates to an improvement in a wave canceling device that reflects and absorbs wave energy. The present inventor filed an application titled "Wave Dissipation/Generation Method" on March 4, 1983, prior to filing this invention, and the present application relates to an improvement thereof.

<発明の構成> 先ず洗顔(潜袋が海中に露出しているもの)を
含めて本願(潜袋を中空円筒で包囲したもの)作
動原理について添付図面の第1図〜第8図を引用
して説明する。第1図は先願に関し潜袋2個を連
通管でつなぎ、波の進行方向に並べて設けたもの
である。aは平面図、bは側面図である。この図
面で11,12は潜袋、2は連通管、Hoは波の
方向、Htは消波された波の方向を示す。第2図
は潜袋4個の場合の側面図、aは海底に固定し、
bは浮遊する台に係留した図、13,14,1
5,16は潜袋、2は連通管である。第3図は先
願における潜袋の作動原理の説明図で、,,
,は波の作用に関する位相別の図面aは側面
図、bは線A−Aに沿う断面図で、4は波の作用
する力の方向、4′はこれによつて生じたひだを
示し、3は潜袋の底に設けた連通管である。
<Structure of the Invention> First, the operating principle of the present application (in which the diving bag is surrounded by a hollow cylinder), including the face wash (in which the diving bag is exposed in the sea), will be described with reference to Figures 1 to 8 of the attached drawings. I will explain. FIG. 1 shows the prior application in which two submersible bags are connected by a communicating tube and arranged side by side in the direction of wave propagation. A is a plan view, and b is a side view. In this drawing, 11 and 12 are submerged bags, 2 is a communication pipe, Ho is the direction of waves, and Ht is the direction of dissipated waves. Figure 2 is a side view of four diving bags, a is fixed to the seabed,
b is a figure moored to a floating platform, 13, 14, 1
5 and 16 are submergence bags, and 2 is a communication pipe. Figure 3 is an explanatory diagram of the operating principle of the diving bag in the earlier application.
, is a phase-by-phase diagram regarding the action of waves. 3 is a communication pipe provided at the bottom of the diving bag.

先ず第3図aは、伸縮性はないが柔軟な膜によ
る潜袋の水中の形状を示す側面図で、は空気を
充満したときの袋の形で、円筒形の上部は半球形
で、下端を固定し、孔3を通して空気が出入す
る。
First, Figure 3a is a side view showing the underwater shape of a diving bag made of a non-stretchable but flexible membrane. is fixed, and air enters and exits through the hole 3.

,,は水中に固定して空気を入れた場合
で、はの空気量の約60%の空気量の場合であ
る。上部は半球状であるが中央部以下はくびれて
ひだ4ができており、その部分のA−A断面を示
すと、bのようである。この状態から空気を抜く
とのようにひだ4′が大きくなつて袋の体積は
減小する。空気を注入するとのようにひだ4は
小さくなり袋の体積は増大する。このように膜面
は伸縮しなくても、ひだが成長または縮少するこ
とによつて、潜袋の体積は容易に増減し、潜袋の
変形が起るのである。
, , is the case where air is fixedly placed in water, and the amount of air is approximately 60% of the amount of air in . The upper part has a hemispherical shape, but the part below the center is constricted to form pleats 4, and the AA cross section of that part is shown in b. When air is removed from this state, the pleats 4' become larger and the volume of the bag decreases. As when air is injected, the pleats 4 become smaller and the volume of the bag increases. In this way, even if the membrane surface does not expand or contract, the volume of the submerged bag can easily increase or decrease due to the growth or contraction of the folds, causing deformation of the submerged bag.

第4図aは間隔Bを以つて波長Lの波の進行方
向に潜袋11及び12を連通していない状態で設
置した場合を示した側面図である。このとき、ほ
ぼ2Bの波長Lをもつ波Hoが入射するとすれば、
潜袋に作用する流体圧力は波の進行と共に変動す
るが、空気は非圧縮性と見なされるから潜袋の体
積は変らず、図のように潜袋11に波峰、潜袋1
2に波底があるときは、水粒子の水平運動により
潜袋にはそれぞれP1及びP2の向きの力が作用し、
静止時に点線で示した形の潜袋は、波の進行によ
つて実線のようにわずかに傾くに止まり、波高
Hoの入射波は潜袋によつて少しばかり阻止され
て反射波高Horを生ずるが、波高はほとんど低減
することなくHotとして通過する。即ち連通しな
い潜袋はほとんど消波機能をもたない。
FIG. 4a is a side view showing a case where the submersible bags 11 and 12 are installed in a state in which they are not in communication with each other in the direction of propagation of waves of wavelength L with a distance B between them. At this time, if a wave Ho with a wavelength L of approximately 2B is incident, then
The fluid pressure acting on the diving bag changes as the wave progresses, but since air is considered incompressible, the volume of the diving bag does not change.
When there is a wave bottom at point 2, forces in the directions P 1 and P 2 act on the diving bag due to the horizontal movement of water particles, respectively.
When at rest, the diving bag shown by the dotted line only tilts slightly as the wave advances, as shown by the solid line, and the wave height increases.
The incident wave Ho is blocked a little by the latent bag and produces a reflected wave height Hor, but the wave height is hardly reduced and passes through as Hot. In other words, a submerged bag without communication has almost no wave-dissipating function.

しかし第4図aの状態においては、潜袋11に
作用している、波による変動圧力は潜袋を圧縮し
ており、潜袋12ではその反対であるから両潜袋
をbのように管2で連通すると、潜袋11の空気
は潜袋12の方に流れて、前者は収縮し後者は膨
脹する。この収縮・膨脹の現象だけを取り出して
考えると、第4図bに示すように、潜袋11付近
の流体は収縮した体積だけ潜袋に向つて集まり、
そのため水面が低下して波底が発生し、一方潜袋
12付近には反対に波峰が発生するが、入射波の
進行にともなつて、この現象が交互に繰り返され
ることになる。即ち両方の潜袋の体積が交互に増
減することによつて、一方に波峰、他方に波底が
交互に現われるという現象が繰り返されて新たな
波HR1とHR2とが誘起され、左右両方に同じ波
高で進行していくことになる。この波を
Radiation Waveと呼ぶ。ここで注意すべきは、
この波は、その原因である第4図aの波の形とは
波峰・波底が逆位相の関係に在ることである。連
通された潜袋では第4図のaとbの状態を重合し
た現象が現われ、潜袋12の右側(通過波側)で
は、図aにおけるHotと同じ方向に進行する、図
bにおけるHR1が重合して相殺される。その結
果波高HtはHotに比べて著しく低くなり、波は
有効にしや断されることとなる。他方潜袋11の
左側(反射波側)では、入射波Hoと、反対方向
に進行するRadiation Wave HR2が重合して波
高が高くなる。(実際には連通管2内の空気流の
エネルギー消滅によりHR2は小さくなり、その
影響は小さい。) 第5図は第4図のaとbを重合した結果を示し
ている。
However, in the state shown in Figure 4a, the fluctuating pressure caused by the waves acting on the diving bag 11 compresses the diving bag, and the opposite is true for the diving bag 12, so both bags are separated into tubes as shown in b. 2, the air in the submergence bag 11 flows toward the submergence bag 12, causing the former to contract and the latter to expand. If we consider only the phenomenon of contraction and expansion, as shown in Fig. 4b, the fluid near the submerged bag 11 gathers toward the submerged bag by the contracted volume,
As a result, the water surface lowers and a wave bottom occurs, while a wave peak occurs near the diving bag 12, and this phenomenon is alternately repeated as the incident wave advances. That is, as the volumes of both submerged bags alternately increase and decrease, the phenomenon of wave peaks appearing alternately on one side and wave bottoms on the other side is repeated, and new waves H R 1 and H R 2 are induced. The waves will proceed at the same height on both the left and right sides. this wave
It is called Radiation Wave. What should be noted here is that
This wave has a wave peak and a wave bottom that are in an opposite phase relationship with the wave shape shown in FIG. 4a, which is the cause of the wave. In the connected submerged bag, a phenomenon that combines the states a and b in Fig. 4 appears, and on the right side of the submerged bag 12 (on the passing wave side), H R in Fig. b, which advances in the same direction as Hot in Fig. 1 polymerizes and cancels each other out. As a result, the wave height Ht becomes significantly lower than Hot, and the waves are effectively cut off. On the other hand, on the left side (reflected wave side) of the diving bag 11, the incident wave Ho and the radiation wave H R 2 traveling in the opposite direction overlap and the wave height increases. (Actually, H R 2 becomes smaller due to energy dissipation of the air flow in the communication pipe 2, and its influence is small.) FIG. 5 shows the result of superimposing a and b in FIG. 4.

結局、潜袋を連通した場合には、その変形によ
り発生するRadiation Waveの波高が大きく、通
過波高Hotに近い程、しや断効果が大きいことに
なる。
After all, when the submersible bag is communicated, the wave height of the radiation wave generated by its deformation is large, and the closer it is to the passing wave height Hot, the greater the shearing effect.

従つて問題は、Radiation Waveを如何に有効
に発生させるか、ということになる。
Therefore, the problem is how to effectively generate radiation waves.

第6図aは静水中でRadiation Waveを発生し
ている潜袋の体積変化と、それにともなう周辺の
流体流速の分布状態を説明するもので、潜袋形状
を表わす鎖線は静止時、実線は膨脹時、破線は収
縮時の形を表わしている。既に第3図にも示した
ように、主な変形は潜袋の下半部に起つており膨
脹時は実線矢印、収縮時は点線矢印のように、流
速はかなり広く拡散分布しているため、水面の上
昇又は低下は余り効果的に起つていないとみられ
る。そこで潜袋周辺の流れを収束させるために上
端を開口した円筒で潜袋を囲んでみると、第6図
bに示すように、流れは潜袋周辺で上昇及び下降
する分布となり、そのために水面の上昇と低下が
効果的に起ることとなる。
Figure 6a illustrates the change in volume of the diving bag that generates radiation waves in still water and the distribution of surrounding fluid flow velocity.The chain line representing the shape of the diving bag is at rest, and the solid line is for expansion. At the time, the broken line represents the shape at the time of contraction. As already shown in Figure 3, the main deformation occurs in the lower half of the submerged bag, and the flow velocity is spread out over a fairly wide range, as shown by the solid line arrow when it is inflated and the dotted line arrow when it is deflated. , it appears that the water level is not rising or falling very effectively. Therefore, if we surround the diving bag with a cylinder with an open top to converge the flow around the diving bag, the flow will have a distribution of rising and falling around the diving bag, as shown in Figure 6b. This effectively results in an increase and decrease in .

第7図は第2図aに示したような、前後に2個
づつの潜袋が連通されている場合について、各々
の潜袋に円筒を設置した効果を、実験によつて示
したものである。即ち直径11cm、空気容積1200
c.c.、高さ21cmのビニル膜による4個の潜袋を、前
後2個づつの潜袋の中間隔を20cm、又それらの中
心間隔B=70cmとして、水深h=35cm、幅W=30
cmの造波水路底に固定し、内径15.0cm、外径16.5
cm、高さ30cmの4本の塩化ビニル管を鉛直筒とし
て用い、入射波高4.0cmに対する通過波高を測定
して、通過波高と入射波高の比(通過率)をKt
とし、その値を縦軸、水深hと波長Lの比を横軸
に取り、実験結果をこのグラフにパレツトしたも
のである。この図の示す点は円筒のみを設置した
場合を×、潜袋のもの場合を●、両者を併用した
場合を○で示したものである。これによつて明ら
かなように、h/L≧0.16において、円筒のみの
場合はKtは約0.7、潜袋のみの場合は約0.6である
が、両者併用の場合は0.3程度となり、0.7×0.6=
0.42の約0.7倍程度であつて、第6図によつて予
測した鉛直円筒の効果は明白である。
Fig. 7 shows the effect of installing a cylinder in each submergence bag through experiments in the case where two submergence bags are connected at the front and back, as shown in Fig. 2a. be. i.e. diameter 11cm, air volume 1200
cc, 4 diving bags made of vinyl membrane with a height of 21 cm, the middle distance between the two diving bags in the front and back is 20 cm, and the center distance between them B = 70 cm, water depth h = 35 cm, width W = 30
Fixed to the bottom of the wave channel with an inner diameter of 15.0 cm and an outer diameter of 16.5 cm.
cm, using four PVC pipes with a height of 30 cm as vertical tubes, measure the passing wave height for an incident wave height of 4.0 cm, and calculate the ratio of the passing wave height to the incident wave height (passage rate) Kt
The experimental results are plotted on this graph, with the value taken as the vertical axis and the ratio of water depth h to wavelength L taken as the horizontal axis. The points shown in this figure are × when only a cylinder is installed, ● when a diving bag is installed, and ○ when both are used together. As is clear from this, when h/L≧0.16, Kt is approximately 0.7 in the case of only the cylinder and approximately 0.6 in the case of only the submerged bag, but it is approximately 0.3 when both are used together, which is 0.7×0.6 =
It is about 0.7 times 0.42, and the effect of the vertical cylinder predicted from FIG. 6 is obvious.

このように潜袋を円筒で囲むことは、消波効果
を向上するに有効であると共に、進行波に伴う水
平方向の流速が直接潜袋に使用してその水平動揺
を発生し、潜袋膜面の耐久性に悪影響を与えるの
を防ぎ、又漂流異物の衝突による潜袋膜の破損を
防止するのに不可欠である。
Surrounding the diving bag with a cylinder in this way is effective in improving the wave-dissipating effect, and the horizontal flow velocity accompanying the traveling wave is directly applied to the diving bag, causing its horizontal oscillation, which causes the diving bag membrane to This is essential to prevent the durability of the surface from being adversely affected and to prevent damage to the diving membrane due to collisions with floating foreign objects.

<実施例> 本願装置の実施態様を第8図乃至第11図を引
用して説明すると次のようである。
<Example> The embodiment of the present device will be described below with reference to FIGS. 8 to 11.

実施例 1 第8図は第1図の潜袋11,12に対して鉛直
円筒5を用いたものである。
Embodiment 1 In FIG. 8, a vertical cylinder 5 is used for the submersible bags 11 and 12 in FIG. 1.

実施例 2 第9図は第2図aの場合に対するもので、前後
2個づつの潜袋13,14と15,16に対して
夫々1個の筒6を用いたもので、このように複数
個の潜袋に共用する1個の筒を用いる方法は、水
平波力に対応するに有利である。
Embodiment 2 FIG. 9 is for the case of FIG. 2a, in which one tube 6 is used for each of the two front and rear submersible bags 13, 14 and 15, 16. The method of using one tube shared by different diving bags is advantageous in dealing with horizontal wave forces.

実施例 3 第10図は第2図bの場合に対する適用の例で
ある。
Embodiment 3 FIG. 10 is an example of application to the case of FIG. 2b.

実施例 4 第11図は第1図の形式を浅海部に用いる場合
の応用例で、aは水平波力に対して筒5を安定に
するためにマウンド7を設けた場合、bは海底を
円筒又は円すい形8に掘り下げて潜袋を設置する
場合を示している。
Embodiment 4 Fig. 11 shows an example of application of the type shown in Fig. 1 in a shallow sea area. A case is shown in which a diving bag is installed by digging into a cylindrical or conical shape 8.

本装置の特徴は、潜袋による没水型消波装置の
特徴をすべて備えている外に、消波効果が時にす
ぐれていること及び潜袋の破損に対する防護が充
分になされていることである。
The features of this device are that in addition to having all the features of a submersible type wave dissipating device using a diving bag, it also has an excellent wave dissipating effect and provides sufficient protection against damage to the diving bag. .

【図面の簡単な説明】[Brief explanation of the drawing]

第1図、第2図、第3図、第4図、第5図及び
第6図は本装置の構成と原理を説明する平面図a
と側面図b、第7図は本装置の原理を証明する実
験結果であり、第8図、第9図、第10図及び第
11図は本装置の実施態様を示す平面図と側面図
である。 11,12,13,14,15,16……潜
袋、2……連通管、3……空気孔、4……潜袋膜
面のひだ、5,6……鉛直円筒及びひだ円筒、7
……マウンド、8……掘り下げ穴、Ho……入射
波、Hr……反射波、Ht……通過波、H……
Radiation Wave。
Figures 1, 2, 3, 4, 5, and 6 are plan views illustrating the structure and principle of this device.
, side view b, and Fig. 7 are experimental results proving the principle of this device, and Figs. 8, 9, 10, and 11 are plan and side views showing embodiments of this device. be. 11, 12, 13, 14, 15, 16... Submerged bag, 2... Communication pipe, 3... Air hole, 4... Folds on the submerged bag membrane surface, 5, 6... Vertical cylinder and pleated cylinder, 7
...Mound, 8...Dug hole, Ho...Incoming wave, Hr...Reflected wave, Ht...Passing wave, H...
Radiation Wave.

Claims (1)

【特許請求の範囲】 1 水面より一定の深さの水中に柔軟な膜を以つ
て適当量の空気を包んだ複数個の袋(以下これを
潜袋という)を波の進行方向に沿つて縦に並べ、
相互の袋を中空管で空気的に連通した消波装置に
おいて、前記潜袋を上端開口した鉛直筒を以つて
囲み、水中に保持したことを特徴とする消波装
置。 2 前記水中の保持が水底に鉛直筒を固定するこ
とによつて行われるようにした特許請求の範囲第
1項に記載の消波装置。 3 前記水中の保持が鉛直筒を固定した台を水底
から水平に係留して行われるようにした特許請求
の範囲第1項に記載の消波装置。
[Claims] 1. A plurality of bags (hereinafter referred to as diving bags) each containing an appropriate amount of air with a flexible membrane are placed vertically in the water at a certain depth below the water surface along the direction of wave propagation. Arrange them in
1. A wave dissipating device in which bags are air-communicated through hollow tubes, characterized in that the submerged bags are surrounded by a vertical tube with an open top and held underwater. 2. The wave dissipating device according to claim 1, wherein the underwater retention is performed by fixing a vertical cylinder to the bottom of the water. 3. The wave dissipating device according to claim 1, wherein the underwater holding is carried out by horizontally mooring a platform to which a vertical cylinder is fixed from the bottom of the water.
JP60124591A 1985-06-08 1985-06-08 Breakwater device Granted JPS62111006A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60124591A JPS62111006A (en) 1985-06-08 1985-06-08 Breakwater device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60124591A JPS62111006A (en) 1985-06-08 1985-06-08 Breakwater device

Publications (2)

Publication Number Publication Date
JPS62111006A JPS62111006A (en) 1987-05-22
JPH0522761B2 true JPH0522761B2 (en) 1993-03-30

Family

ID=14889245

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60124591A Granted JPS62111006A (en) 1985-06-08 1985-06-08 Breakwater device

Country Status (1)

Country Link
JP (1) JPS62111006A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2639577B2 (en) * 1988-12-22 1997-08-13 株式会社間組 Wave absorber
JP6997497B2 (en) * 2018-01-15 2022-01-17 芦森工業株式会社 Tsunami control method and equipment

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