JPS6048632B2 - Float type wave power generation device - Google Patents

Float type wave power generation device

Info

Publication number
JPS6048632B2
JPS6048632B2 JP52124096A JP12409677A JPS6048632B2 JP S6048632 B2 JPS6048632 B2 JP S6048632B2 JP 52124096 A JP52124096 A JP 52124096A JP 12409677 A JP12409677 A JP 12409677A JP S6048632 B2 JPS6048632 B2 JP S6048632B2
Authority
JP
Japan
Prior art keywords
float
wave
power generation
waves
generation device
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
Application number
JP52124096A
Other languages
Japanese (ja)
Other versions
JPS5458151A (en
Inventor
潔 井上
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.)
Inoue Japax Research Inc
Original Assignee
Inoue Japax Research Inc
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 Inoue Japax Research Inc filed Critical Inoue Japax Research Inc
Priority to JP52124096A priority Critical patent/JPS6048632B2/en
Publication of JPS5458151A publication Critical patent/JPS5458151A/en
Publication of JPS6048632B2 publication Critical patent/JPS6048632B2/en
Expired 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
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/30Energy from the sea, e.g. using wave energy or salinity gradient

Landscapes

  • Other Liquid Machine Or Engine Such As Wave Power Use (AREA)

Description

【発明の詳細な説明】 本発明は浮子式の波力発電装置に関する。[Detailed description of the invention] The present invention relates to a float-type wave power generation device.

海上に錨をもつて浮枠を固定し、これに波浪で上下する
浮子と、電動機と上記浮子の上下運動を回転運動に変換
し上記発電機に入力させる運動変換装置を設けて成る浮
子式波力発電装置は公知てある。
A float-type wave consisting of a floating frame fixed with an anchor on the sea, which is equipped with a float that moves up and down with the waves, an electric motor, and a motion conversion device that converts the up-and-down motion of the float into rotational motion and inputs it to the generator. Power generating devices are known.

この公知の発電装置を有効に作動させるためには浮枠を
確実に固定させると共に、該浮枠によつて昇降自在に支
承される浮子が波浪により円滑に、かつ効率よく上下で
きるようにする必要がある。
In order to effectively operate this known power generation device, it is necessary to securely fix the floating frame, and also to ensure that the float, which is supported by the floating frame so as to be able to rise and fall, can move up and down smoothly and efficiently due to waves. There is.

浮枠の固定には錨索と錨が用いられる。Anchor lines and anchors are used to secure the floating frame.

また、浮子の形状については一般に円柱または円板形の
ものが多く使用されるが、従来公知のものでは浮子を効
率よく上下動させ難く、そのため発電効率を高めること
ができなかつた。本発明は叙上の観点に立つてなされた
ものであり、その目的とするところは、波浪エネルギを
有効に利用できるよう改良された浮子を具えた発電効率
の高に波力発電装置を提供することにある。
In addition, although cylindrical or disc-shaped floats are generally used, conventionally known floats have difficulty in efficiently moving the float up and down, making it impossible to increase power generation efficiency. The present invention has been made based on the above-mentioned viewpoints, and its purpose is to provide a wave power generation device with high power generation efficiency, which is equipped with an improved float so that wave energy can be effectively utilized. There is a particular thing.

而して、本発明の要旨とするところは、浮子の厚みを波
の進行方向に順次増大するよう構成し、波浪作用時の浮
子に作用する外力を波の進行方向に沿つての浮子の前後
で平衡せしめ、波浪エネルギを有効に利用し、発電効率
を高めることにある。なお、通常この波力発電装置が設
けられるのは、海岸に近い所であり、そこでは通常波が
沖合から海岸に向かうものであるから、本発明の以下の
説明においては、特に断らない限りそのように扱うが、
必ずしもそのような場合に限られるものではなく、波の
進行方向はどのような方向であつてもよく、また、その
進行方向が随時変化するような場合でも本発明を実施し
得ることは勿論である。
Therefore, the gist of the present invention is that the thickness of the float is configured to increase gradually in the direction of wave propagation, and the external force acting on the float during wave action is applied to the float before and after the float in the direction of wave propagation. The objective is to balance the waves, use wave energy effectively, and increase power generation efficiency. Note that this wave power generation device is usually installed near the coast, where waves usually travel from offshore to the coast, so in the following description of the present invention, unless otherwise specified, such However,
The present invention is not necessarily limited to such a case, and the direction of travel of the waves may be any direction, and it goes without saying that the present invention can be carried out even in cases where the direction of travel changes from time to time. be.

以下図面により本発明の詳細を説明する。The details of the present invention will be explained below with reference to the drawings.

第1図は本発明にかかる波力発電装置の一実施例を示す
側面図であり、第2図はその平面図、第3図は・従来の
波力発電装置に使用されていた浮子の波浪時の状態を示
す説明図、第4図は本発明にかかる波力発電装置に使用
される浮子の波浪時の状態を示す説明図、第5図は第4
図に示す浮子が浮上して傾いた状態を示す図、第6図は
浮子が回動した・状態を示す浮子の平面図、第7図は第
6図のe一g断面図である。而して、図中1は浮枠、2
は浮子、3及び4は案内車輪、5は発電機その他が収容
されている機械室、6は浮子2に固着した昇降軸、7は
錨、8は錨索、9は波面である。
FIG. 1 is a side view showing an embodiment of the wave power generation device according to the present invention, FIG. 2 is a plan view thereof, and FIG. FIG. 4 is an explanatory diagram showing the state of the float used in the wave power generation device according to the present invention during waves, and FIG.
FIG. 6 is a plan view of the float showing a rotated state, and FIG. 7 is a sectional view of e-g in FIG. 6. Therefore, 1 in the figure is a floating frame, 2
1 is a float, 3 and 4 are guide wheels, 5 is a machine room in which a generator and others are housed, 6 is a lifting shaft fixed to the float 2, 7 is an anchor, 8 is an anchor cable, and 9 is a wave surface.

浮枠1は、主柱1a,1a,粱1b,1c,1d等から
成る直方形又は円筒形等の浮体であり、軽質材で製作さ
れるか、又は適宜の浮きが取付けられて海上に浮かべら
れ、錨7及び錨索8により、または、必要に応じさらに
ダンパを介して固定される。
The floating frame 1 is a rectangular or cylindrical floating body consisting of main pillars 1a, 1a, rods 1b, 1c, 1d, etc., and is made of light material or is floated on the sea with appropriate floats attached. It is fixed by the anchor 7 and the anchor cable 8, or further via a damper if necessary.

浮子2は、浮枠1の主柱1a,1aに沿つて走行し得る
案内車輪3及び4を介して、浮枠1に昇降自在に支承さ
れており波面の上下に応じて昇降J軸6と共に上下する
The float 2 is supported by the floating frame 1 so as to be able to rise and fall through guide wheels 3 and 4 that can run along the main pillars 1a and 1a of the floating frame 1, and moves up and down along with the J axis 6 according to the up and down of the wave surface. Go up and down.

浮子2に固着した昇降軸6は、浮子2の上下運動を機械
室5内の機器に伝達する軸である。機械室5内には公知
の発電機、上記昇降軸6の上下運動を発電機に伝達する
運動変換装置、蓄電器、蓄電池、送電設備及ひ各種の電
力消費機器等が設けられている。
A lift shaft 6 fixed to the float 2 is a shaft that transmits the vertical movement of the float 2 to equipment in the machine room 5. In the machine room 5, there are provided a known generator, a motion conversion device for transmitting the vertical movement of the lifting shaft 6 to the generator, a power storage device, a storage battery, power transmission equipment, various power consumption devices, and the like.

而して、上記運動変換装置には、例えば、往復動ピスト
ン式若しくは回転ピストン式のエアコンプレッサとエア
タービンから成るもの、又はワンウェイクラッチ、フラ
イホィール及び無段変速機等から成るもの等が知られて
いる。また、浮子2としては、太く短い円柱形のものを
示したが、細長い円柱形のものも使用でき、またその浮
沈の自由振動数を波の振動数と一致させておけば波高値
以上の上下動振幅が得られるものである。而して、本発
明の要旨とするところは、浮子の厚みを波の進行方向に
順次増大するよう構成し、波浪作用時の浮子に作用する
外力を沖合側と海岸側とで平衡せしめ、よつて浮子の運
動を円滑なら.しめ、波浪エネルギを有効に利用するこ
と、即ち波浪エネルギが円滑に発電機に伝達されるよう
にすることにある。
As the above-mentioned motion converting device, for example, one consisting of a reciprocating piston type or rotary piston type air compressor and an air turbine, or one consisting of a one-way clutch, a flywheel, a continuously variable transmission, etc. are known. ing. In addition, as the float 2, although a thick and short cylindrical one is shown, an elongated cylindrical one can also be used, and if the free frequency of floating and sinking is made to match the frequency of the waves, the float will rise and fall above the wave height. The dynamic amplitude can be obtained. The gist of the present invention is that the thickness of the float is configured to increase gradually in the direction of wave propagation, and the external force acting on the float during wave action is balanced between the offshore side and the shore side. If the movement of the float is smooth. The objective is to use wave energy effectively, that is, to ensure that wave energy is smoothly transmitted to the generator.

浮子の厚みが均一であると、第3図に示す如く、浮上時
に波浪による浮力は、先ず昇降軸6を一浮子10に取付
けた口の点を中心に考えた場合に、浮子10を矢印Aの
方向に回転するように作用する。
If the thickness of the float is uniform, as shown in FIG. It acts to rotate in the direction of.

この矢印Aの回転力は水平な波面9,9’と浮子10と
が交わる図中イ,ト,ホ。へに囲まれた部分の波浪の体
積に比例し、この矢印A・の回転力に釣り合う方向に働
く矢印Bの回転力は図中卜,二,ホに囲まれた部分の体
積に比例する1から、両者の回転力、A,Bが釣り合う
のは浮子10のイの点の波面9がハの点に達したときで
あ :る。即ち昇降軸6を軸方向に押す均一なりは、波
浪の波面9が浮子10を覆うときに初めて得られ、しか
も回転力Aで傾いた浮子10を復元する力は浮子10の
傾きによる重心の移動にともなう浮力のみによるという
欠点があつた。而して、叙上の如く浮子2の上面または
下面の少くとも一方を傾斜面とし、沖合側に対し海岸側
の浮力を大きくしてやれば波浪による浮力が効率よく浮
子の上下動につながり、その結果発電効果が高められる
ものである。
The rotational force indicated by arrow A is expressed by points A, T, and H in the figure where the horizontal wave surfaces 9 and 9' intersect with the float 10. The rotational force of arrow B, which acts in a direction that balances the rotational force of arrow A, is proportional to the volume of the waves in the area surrounded by 1, 2, and 1 in the figure. Therefore, the rotational forces A and B are balanced when the wavefront 9 at point A of the float 10 reaches point C. In other words, the ability to push the lifting shaft 6 in the axial direction can only be obtained when the wave front 9 of the waves covers the float 10, and the force that restores the float 10 tilted by the rotational force A is due to the movement of the center of gravity due to the tilt of the float 10. The drawback was that it relied solely on the buoyancy associated with the movement. Therefore, as mentioned above, if at least one of the top or bottom surfaces of the float 2 is made sloped, and the buoyancy on the shore side is made larger than on the offshore side, the buoyancy caused by the waves will efficiently lead to the vertical movement of the float, and as a result. This increases the power generation effect.

即ち、浮子2に作用する波浪、特に下降位置にある浮子
2に作用して該浮子を上昇させる波浪は、海岸側から沖
合側にかけて高くなるように傾斜した波面の海岸側へ向
けての平行移動であるから、浮子2に対する浮力は沖合
側から、また海岸側よりも沖合側の方が大きい関係で作
用し、このため浮子2を沖合側が高くかつ海岸側が低く
なるように変位傾斜せしめ、浮子2の円滑な上昇を阻害
する可能性があるが、本発明によれば、第4図に示す如
く、浮子2を海岸側が高く、かつ沖合側が低くなるよう
に変位傾斜せしめて、浮子2の沖合側の体積を小さくし
、反対に海岸側の体積を大きくすることによつて、波浪
の傾斜した波面9が昇降軸6を浮子10に取付けたり点
に達し、傾斜した波面9の先端が、水平な波面9,9’
と浮子2とが交わるル点に達したときには、チ,り,オ
で囲まれた部分の体積と、り,ル,オで囲まれた部分の
体積とが同じになる。
In other words, the waves acting on the float 2, especially the waves acting on the float 2 in the lowered position and raising the float, are caused by the parallel movement of the wave surface, which slopes upward from the shore side to the offshore side, toward the shore side. Therefore, the buoyant force on the float 2 acts from the offshore side, and is greater on the offshore side than on the coast. Therefore, the float 2 is displaced and tilted so that the offshore side is higher and the coast side is lower. However, according to the present invention, as shown in FIG. By reducing the volume of the wave surface and increasing the volume on the shore side, the inclined wave surface 9 of the wave reaches the point where the lifting shaft 6 is attached to the float 10, and the tip of the inclined wave surface 9 becomes horizontal. Wave surface 9,9'
When the point R is reached, where and the float 2 intersect, the volume of the part surrounded by Chi, Ri, and O becomes the same as the volume of the part surrounded by Ri, Ru, and O.

従つて、り点を中心に回転モーメントC,Dを考えると
、回転モーメントCを生じるチ,り,オで囲まれた部分
の体積と、回転モーメントDを生じるり,ル,オで囲ま
れた部分の体積が同じになるから回転モーメントC,D
が均衡することになる。波浪は沖合側が高く、海岸側が
低くなるように傾斜して押し寄せてくるものであるから
、それにより浮子2に側方から加わる水平方向の波浪の
圧力、つまり波力があるが、それを無視すると浮子2は
浮力的には水平を保つて上昇して昇降軸6を効率よく上
昇させる。一方、波浪は第5図に示すように、鎖線で示
すG位置から実線で示すH位置に移動する。
Therefore, considering the rotational moments C and D around point ri, the volume of the part surrounded by ri, ri, and o that produces the rotational moment C, and the volume of the part surrounded by ri and o that produces the rotational moment D. Since the volumes of the parts are the same, the rotational moments C and D
will be in equilibrium. Waves are higher on the offshore side and lower on the shore side, so there is horizontal wave pressure, or wave force, that is applied to the float 2 from the sides, but if we ignore this, The float 2 rises while remaining horizontal in terms of buoyancy, and efficiently raises the lifting shaft 6. On the other hand, as shown in FIG. 5, the waves move from the G position shown by the chain line to the H position shown by the solid line.

この移動する波浪の斜面によつて上昇した浮子2は実線
で示したチ′,り′,ヌ′,ル′のように傾くが、この
とき浮子2のチ′,り′を結ふ線より上を進行する波浪
は浮子2の浮力となる影響を及ぼさないから、波浪がり
′,ル′を結ぶ線より上の部分を進行することによつて
生じた浮力は傾いた浮子2を含む浮枠1の復元力になる
。更に、波浪が高く、激しく、急傾斜になると、それに
従つて浮子2の傾きが急で、しかも大きくなるが、浮子
2のり’,ヌ′,ル′で囲む部分を進行する波浪の量も
多くなり、それに比例して浮子2の復元力が増大するか
ら、その増大した復元力によつて速やかに浮子2を含む
浮枠1の傾きを復元し、水平に浮上した位置で安定する
。又、浮子2の厚みは沖合側より海岸側が厚くなるよう
に上面が傾斜しているから、浮子2を上方から視た平面
図である第6図で示すように、浮子2の同じ厚さの部分
を示す、所謂等高線Efが、波浪の進向方向を示す矢印
Fに対して傾斜するように浮子2が半時計方向に回動し
たとすると、浮子2を、e点における矢印Fに対する直
角方向のEgに沿つて断面したときのF矢視断面は、第
7図に示すように傾斜した断面になる。
The float 2, which has risen due to the slope of the moving waves, tilts as shown by the solid lines CH', R', N', R', but at this time, the float 2 is tilted from the line connecting CH', R' Since the waves traveling above do not have any effect on the buoyancy of the float 2, the buoyant force generated by the waves traveling above the line connecting the waves ′ and ru′ will affect the floating frame including the tilted float 2. 1 resilience. Furthermore, as the waves become higher, stronger, and steeper, the inclination of the float 2 becomes steeper and larger, but the amount of waves traveling through the area surrounded by the float 2', ``nu'', and ``ru'' also increases. Since the restoring force of the float 2 increases in proportion to this, the increased restoring force quickly restores the inclination of the floating frame 1 including the float 2 and stabilizes it in a horizontally floating position. Furthermore, since the upper surface of the float 2 is inclined so that it is thicker on the shore side than on the offshore side, as shown in Figure 6, which is a plan view of the float 2 seen from above, the thickness of the float 2 is Assuming that the float 2 is rotated counterclockwise so that the so-called contour line Ef that indicates the wave direction is inclined with respect to the arrow F that indicates the direction of wave movement, the float 2 is rotated in a direction perpendicular to the arrow F at point e. The cross section taken along the Eg line is an inclined cross section as shown in FIG.

従つて、この断面部分に加わる波浪の圧力で、浮子2を
側方より押す力は断面積がg点よりe点に向かつて増大
する結果、e点に於てP矢示したような浮子2に対する
回動力を生じ、浮子2を第6図に於て時計方向に回動す
る。そして、等高線Efが波浪の進行方向を示す矢印F
と直角になつたところで波浪の圧力が平均して静止する
。つまり浮子2の厚さの薄い先端が常時沖合側に向くよ
うに浮子2を安定させる。 なお、浮子2の下降は波浪
の通過に従つて、また通過後浮子2の自重により、或る
程度時間をかけて行なわれるものであるから格別問題は
ない。然しながら、この浮子の上下面の傾斜角は、波力
発電装置の設置場所の気象、海象条件、特に波浪の傾斜
角度、周期、振幅、波長等のほか浮枠1 ιおよび浮子
2の構造、形状、寸法、材質、錨索取付部8aの位置等
々を勘案して適切に決定する必要がある。
Therefore, due to the pressure of waves applied to this cross-sectional area, the force pushing the float 2 from the side increases as the cross-sectional area moves from point g to point e. A rotational force is generated against the rotational force, and the float 2 is rotated clockwise in FIG. Then, the contour line Ef is an arrow F indicating the direction of movement of the waves.
When the wave becomes perpendicular to the wave, the pressure of the wave averages out and becomes stationary. In other words, the float 2 is stabilized so that the thin tip of the float 2 always faces offshore. Incidentally, there is no particular problem since the lowering of the float 2 takes a certain amount of time as the waves pass and due to the weight of the float 2 after passing. However, the inclination angle of the upper and lower surfaces of the float depends on the weather and sea conditions of the installation location of the wave power generation device, especially the inclination angle, period, amplitude, wavelength, etc. of the waves, as well as the structure and shape of the floating frame 1 and the float 2. , it is necessary to appropriately determine the size, material, position of the anchor cable attachment part 8a, etc.

本発明は叙上の如く構成されるから、本発明によるとき
は、波浪エネルギが有効に利用でき、それ故発電効率の
高に波力発電装置を提供できるものである。
Since the present invention is constructed as described above, according to the present invention, wave energy can be used effectively, and therefore a wave power generation device with high power generation efficiency can be provided.

なお、浮枠1の下部に鉛直な翼弦を有する多数の平行翼
からなる翼列を設けると浮枠1の揺動を抑制でき、さら
に効率的な発電が可能となる。
In addition, if a blade row consisting of a large number of parallel blades having a vertical chord is provided at the lower part of the floating frame 1, the swinging of the floating frame 1 can be suppressed, and even more efficient power generation becomes possible.

また、本発明の発電装置を波浪の進行方向が常に一定な
海岸近くではなく、季節や気象状態により変化する太洋
中に浮設する場合には、波浪の進行方向の変化に応じ浮
枠1または浮子2を所望の角度、好ましくは自動的に回
動制御設定する必要がある。そして、浮子2の上下面の
少くとも一方の傾斜面は、前述の如く連続的に滑らかな
傾斜面とすることが望ましいものの、場合によつては、
別異の階段形状、或いはさらに別途の浮子や重錘等の付
設による部分的浮力調節等を行なうことを妨たげるもの
ではない。
In addition, when the power generation device of the present invention is floating in the ocean where the direction of wave movement changes depending on the season and weather conditions, rather than near the coast where the direction of movement of waves is always constant, the floating frame 1 Alternatively, it is necessary to set the float 2 to a desired angle, preferably automatically controlling the rotation. Although it is desirable that at least one of the upper and lower surfaces of the float 2 be a continuous and smooth slope as described above, in some cases,
This does not preclude partial buoyancy adjustment by using a different staircase shape or by adding a separate float or weight.

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

第1図は、本発明にかかる波力発電装置の一実・施例を
示す一側面図てあり、第2図はその平面図第3図は従来
の波力発電装置に使用されていた浮子の波浪時の状態を
示す説明図、第4図は本発明にかかる波力発電装置に使
用される浮子の波浪時の状態を示す説明図、第5図は第
4図に示す浮子フが浮上して傾いた状態を示す図、第6
図は浮子が回動した状態を示す浮子の平面図、第7図は
第6図のe−g断面図である。 1 ・・・・・・浮枠、2 ・・・・・・浮子、3,4
・・・・・・案内車輪、5・・・・・・機械室、6・・
・・・・昇降軸、7・・・・・・錨、89・・・・・・
錨索、9・・・・・・波面。
FIG. 1 is a side view showing an embodiment of the wave power generation device according to the present invention, FIG. 2 is a plan view thereof, and FIG. 3 is a float used in a conventional wave power generation device. FIG. 4 is an explanatory diagram showing the state of the float used in the wave power generation device according to the present invention during waves, and FIG. Figure 6 showing the tilted state
The figure is a plan view of the float showing the state in which the float is rotated, and FIG. 7 is a sectional view taken along the line e-g in FIG. 6. 1...Floating frame, 2...Float, 3,4
...Guide wheel, 5...Machine room, 6...
... Lifting axis, 7 ... Anchor, 89 ...
Anchor cable, 9...Wave surface.

Claims (1)

【特許請求の範囲】[Claims] 1 海上の所望の位置に錨で固定される浮枠と、上記浮
枠により昇降自在に支承された浮子と、上記浮枠上に設
けられた発電機と、上記浮子の上下運動を上記発電機の
入力軸回転運動に転換し得る運動変換装置とから成る浮
子式波力発電装置において、浮子の厚みが、波の進行方
向に順次増大するよう構成されたことを特徴とする上記
の浮子式波力発電装置。
1. A floating frame fixed to a desired position on the sea with an anchor, a float supported by the floating frame so as to be able to rise and fall freely, a generator installed on the floating frame, and a generator that controls the vertical movement of the float. and a motion conversion device capable of converting the rotational motion of the input shaft into rotational motion of the input shaft, the above-mentioned rotatable wave power generation device is characterized in that the thickness of the float is configured to increase sequentially in the direction of wave propagation. power generator.
JP52124096A 1977-10-18 1977-10-18 Float type wave power generation device Expired JPS6048632B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP52124096A JPS6048632B2 (en) 1977-10-18 1977-10-18 Float type wave power generation device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP52124096A JPS6048632B2 (en) 1977-10-18 1977-10-18 Float type wave power generation device

Publications (2)

Publication Number Publication Date
JPS5458151A JPS5458151A (en) 1979-05-10
JPS6048632B2 true JPS6048632B2 (en) 1985-10-28

Family

ID=14876814

Family Applications (1)

Application Number Title Priority Date Filing Date
JP52124096A Expired JPS6048632B2 (en) 1977-10-18 1977-10-18 Float type wave power generation device

Country Status (1)

Country Link
JP (1) JPS6048632B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62140323A (en) * 1985-12-13 1987-06-23 株式会社明電舎 Vacuum interruptor

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62140323A (en) * 1985-12-13 1987-06-23 株式会社明電舎 Vacuum interruptor

Also Published As

Publication number Publication date
JPS5458151A (en) 1979-05-10

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