[go: up one dir, main page]

JP2013036365A - Ocean energy power generation system - Google Patents

Ocean energy power generation system Download PDF

Info

Publication number
JP2013036365A
JP2013036365A JP2011171413A JP2011171413A JP2013036365A JP 2013036365 A JP2013036365 A JP 2013036365A JP 2011171413 A JP2011171413 A JP 2011171413A JP 2011171413 A JP2011171413 A JP 2011171413A JP 2013036365 A JP2013036365 A JP 2013036365A
Authority
JP
Japan
Prior art keywords
current
ocean
currents
tidal
power generation
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.)
Withdrawn
Application number
JP2011171413A
Other languages
Japanese (ja)
Inventor
Noriaki Fujimura
紀明 藤村
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to JP2011171413A priority Critical patent/JP2013036365A/en
Publication of JP2013036365A publication Critical patent/JP2013036365A/en
Withdrawn legal-status Critical Current

Links

Images

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
    • Y02E10/20Hydro energy
    • 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

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

Abstract

PROBLEM TO BE SOLVED: To provide an ocean current and tidal current wave power generation system which can sensitively and optimally respond to complicated motions of ocean currents and tidal currents in a wide range and has a large size and outputs high power with high efficiency and is economical.SOLUTION: Rotary disks 11, 12 are mounted with a large number of current-receiving blades 3 which have faces in a vertical direction and are arranged in a passive variable pitch or a fixed pitch of a lifting force generation type or an active variable pitch. The rotary disks are installed in a horizontal direction near the water surface or tethered to float, and made to rotate by acquiring a propelling force in the same direction from motions of ocean currents and tidal currents as an energy source, and thereby, energy is absorbed from the rotation. By mounting a large number of current-receiving blades on segmented positions, it is possible to respond with an independent and optimal form in each segment to a water flow that always changes in accordance with the motion directions and flow velocities of ocean currents and tidal currents and influences of other blades, and as the whole apparatus, a current receiving cross-sectional area with respect to ocean currents and tidal currents can be increased in size and the structure can be simplified.

Description

本発明は、海洋エネルギーを利用する海流・潮流発電方式に関するものである。 The present invention relates to an ocean current / tidal current power generation system using ocean energy.

自然エネルギーを利用した発電は化石燃料によらない発電方式として、地球温暖化防止、資源の偏在対策、経済浮揚効果など、その期待効果は大きい。 Power generation using natural energy is a power generation method that does not rely on fossil fuels, and it has great expectations such as prevention of global warming, measures against uneven distribution of resources, and effects of economic levitation.

海洋エネルギーを利用した発電としては、海流発電、潮流発電、波浪発電、温度差発電等があるが、それぞれ賦存量は大きい。その中でも海流、潮流は、波浪に比べて存在する地域が限られているものの、エネルギー密度は大きく大いに利用価値がある。
しかしながら従来提案されている海流発電、潮流発電方式は、規模も小さく、設置も困難であり、発電コストも高く、大規模な商業レベルでの実用化を行うには十分ではなかった。
As power generation using ocean energy, there are ocean current power generation, tidal current power generation, wave power generation, temperature difference power generation, and the like, but their existing amounts are large. Among them, ocean currents and tidal currents are limited in the area where they exist compared to waves, but the energy density is large and has great utility value.
However, the ocean current power generation and tidal current power generation methods that have been proposed in the past are small in scale, difficult to install, high in power generation cost, and not sufficient for practical use at a large commercial level.

実用化を進めるためには、技術面からは大型化、高効率化をすすめること、コスト面からは建設コスト、発電コストを低減することが必須である。 In order to promote practical application, it is essential to increase the size and increase the efficiency from the technical aspect and to reduce the construction cost and power generation cost from the cost aspect.

海流は偏西風等の風により生ずる大洋の大循環流であり、ほぼ一定の方向に流れる。しかしながら、海流の強い地点は陸地から数Km以上離れており、大水深であるため装置の設置や管理が難しく、潮流発電に類似する従来の方式では発電システムを実現するのは難しかった。 Ocean currents are oceanic circulations caused by winds such as westerly winds, and flow in almost constant directions. However, the point where the ocean current is strong is several kilometers away from the land, and it is difficult to install and manage the equipment because of the deep water depth, and it was difficult to realize the power generation system with the conventional method similar to tidal current power generation.

潮流発電は潮の干満によって引き起こされるによって起こる流れを利用するもので、潮流を利用できる場所は陸地から比較的近く、海流に比べれば発電システムの設置はしやすい。ただし流れの方向は日に2回反転する。 Tidal current power generation uses the flow caused by tidal currents, and the location where the tidal current can be used is relatively close to the land, making it easier to install a power generation system than ocean currents. However, the direction of flow is reversed twice a day.

従来の海流、潮流発電の方式には以下の例がある。 Examples of conventional ocean current and tidal current power generation methods are as follows.

ひとつは水平軸型タービンとして分類されるものであり、代表的な例はプロペラ式であり水中に設置された羽が海流、潮流の流れを受けて回転し発電機を駆動する。 One is classified as a horizontal axis turbine. A typical example is a propeller type, and the wings installed in the water rotate in response to the flow of ocean currents and tidal currents to drive the generator.

他のひとつは垂直軸型タービンとして分類されるものであり、例としてダリウス型、サボニウス式がある。 The other is classified as a vertical axis turbine, and examples include Darius type and Savonius type.

しかしながらこれらの方式はプロペラの大型化が困難であり、設置も困難であり、発電システムを低コストで大型化をするのは困難であった。 However, these methods are difficult to increase the size of the propeller, are difficult to install, and it is difficult to increase the size of the power generation system at low cost.

特開2011−117397JP2011-117397A

「NEDO再生可能エネルギー技術白書」新エネルギー・産業技術総合開発機構(NEDO)2010年12月"NEDO Renewable Energy Technology White Paper" New Energy and Industrial Technology Development Organization (NEDO) December 2010

発明が解決しようとする課題は、効率のよい大型大出力の経済的な海流、潮流発電システムを提供することである。 The problem to be solved by the present invention is to provide an efficient large-scale and large-output economical ocean current and tidal current power generation system.

具体的には、海流、潮流に対する受流断面積または受流線長を大きくとること、運動方向や大きさが変化する海流、潮流にきめこまかく対応できる方式を実現すること、エネルギー吸収の高効率化を実現することである。 Specifically, the receiving cross-sectional area or the receiving line length for ocean currents and tidal currents is increased, the ocean currents that change in the direction and size of movement, the method capable of finely responding to tidal currents, and the high efficiency of energy absorption. Is to realize.

また装置自身を含む建設費、保守費、発電コストの安い方式を提供することであり、そのためには、構造が簡潔で、製造、運搬、設置が容易な方式を実現すること、特に海流、潮流が大きく設置面積が大きくとれる沖合での設置の簡潔化を実現することである。 In addition, it is to provide a system with low construction costs, maintenance costs, and power generation costs, including the equipment itself, and to realize a system that is simple in structure, easy to manufacture, transport, and install, especially ocean currents and tidal currents. It is to realize the simplification of the installation offshore where the installation area can be large.

上記の目的を達成するために、本発明は以下の手段を提供する。 In order to achieve the above object, the present invention provides the following means.

本発明の海流、潮流発電方式は、面の向きが垂直方向の多数の受動可変ピッチまたは多数の揚力発生型の固定ピッチまたは多数の能動可変ピッチの受流翼を装備した回転盤を水面付近の水平の方向に設置し、または浮揚繋留させ、エネルギー源である海流、潮流運動から推進力を得て回転させ、この回転からエネルギーを吸収する。 The ocean current and tidal current power generation method according to the present invention is a method of turning a rotary disk equipped with a plurality of passive variable pitches whose vertical direction is vertical, a large number of lift generating fixed pitches or a large number of active variable pitch receiving vanes near the water surface. It is installed in the horizontal direction or is levitated and tethered, and it is rotated by obtaining a propulsive force from the ocean current and tidal motion that are energy sources, and absorbs energy from this rotation.

本発明によれば、区分化された位置に多数の受流翼を装備することにより、海流、潮流の運動方向や大きさの絶えず変化する水流に対して、各区分毎に独立かつ最適な形体で対応でき、装置全体として広範囲の海流、潮流の複雑な運動にきめ細かく最適に対応される。 According to the present invention, by installing a large number of receiving wings at the segmented positions, independent and optimal features for each segment with respect to the ocean currents and the water currents that constantly change in the direction and size of the tidal currents. The system as a whole can handle a wide range of ocean currents and complex tidal currents in a fine and optimal manner.

本発明によれば、垂直方向に装備された各受流翼を受動型の可変ピッチ型、または能動型の可変ピッチ型、また揚力発生型の固定ピッチにすることにより、海流、潮流の方向が、時間、位置により変化しても海流、潮流による円盤の回転推進方向は同一であり、同一方向の回転運動が行わる。 According to the present invention, the direction of the ocean current and the tidal current can be adjusted by making each receiving blade installed in the vertical direction a passive variable pitch type, an active variable pitch type, or a lift generating type fixed pitch. Even if it changes with time and position, the rotational propulsion direction of the disk by the ocean current and tidal current is the same, and the rotational movement in the same direction is performed.

本発明によれば、装置全体は着底型でも繋留された浮体型でも良く、設置場所選択の自由度が大きく、運搬、設置工事も簡単である。特に海流、潮流が大きく、広い設置面積がとれる沖合での設置を可能とする。 According to the present invention, the entire apparatus may be a bottomed type or a tethered floating type, has a high degree of freedom in selecting an installation location, and is easy to carry and install. In particular, ocean currents and tidal currents are large, enabling installation offshore with a large footprint.

本発明によれば、広い回転盤の構造を簡単にでき、また適切な浮力を与えることができ、重力に対抗するための強固な構造にする必要がなく、簡単な構造で大型化を可能とする。 According to the present invention, the structure of a wide rotating disk can be simplified, an appropriate buoyancy can be given, and it is not necessary to make a strong structure to resist gravity, and it is possible to increase the size with a simple structure. To do.

本発明により以下のような効果が生ずる。 The following effects are produced by the present invention.

垂直方向に装備された各受流翼を受動型の可変ピッチ型、または能動型の可変ピッチ型、また揚力発生型の固定ピッチの受流翼を区分化した位置に装備することにより、海流、潮流の運動方向や大きさの絶えず変化する波流に対して、各区分毎に独立かつ最適な形体で対応でき、装置全体として広範囲の海流、潮流の複雑な運動にきめ細かく最適に対応できる。 By installing each receiving blade installed in the vertical direction to a passive variable pitch type, or an active variable pitch type, and a lift generating type fixed pitch receiving blade at a segmented position, It is possible to respond to wave currents that constantly change in the direction and size of tidal currents in an independent and optimal form for each section, and the entire device can be optimally adapted to a wide range of ocean currents and complex tidal currents.

また、各受流翼は海流、潮流の方向が、時間、位置により変化しても海流、潮流による円盤の回転推進方向は同一であり、同一方向の回転運動が行われ、安定した発電動作が実現できる。 In addition, even if the direction of the ocean current and tidal current changes depending on the time and position, the receiving blades have the same rotational propulsion direction of the disk due to the ocean current and tidal current. realizable.

また、広い回転盤は構造が簡単であり適切な浮力を与えることができ、重力に対抗するための強固な構造にする必要がなく、大型化が容易である。 In addition, a wide rotating disk has a simple structure, can give an appropriate buoyancy, and does not need to be a strong structure to resist gravity, and can be easily increased in size.

また、装置全体を着底型のみならず繋留された浮体型にできるので、設置場所選択の自由度が大きく、運搬、設置工事も簡単である。特に海流、潮流流力が大きく大出力の発電が期待でき、また広い設置面積がとれる沖合での設置が可能であるので、システムの大規模化、設置場所取得の低コスト化、住民問題回避、漁業問題回避が図れる。 In addition, since the entire apparatus can be a floating type that is anchored as well as a bottomed type, the degree of freedom in selecting the installation location is large, and transportation and installation are easy. In particular, it can be expected to generate large-scale power generation with large ocean currents and tidal currents, and can be installed offshore with a large installation area. The fishery problem can be avoided.

また、回転盤はほぼ水面付近または水面下にあるので、風力発電のような騒音問題、鳥の衝突死問題、景観問題を引き起こすことはない。回転盤の回転速度は風力発電の翼程の高速ではないので、遠心力による破壊や海洋の動物の衝突死問題を引き起こす可能性は少ない。 Moreover, since the rotating disk is almost near or below the surface of the water, it does not cause noise problems such as wind power generation, bird crash death problems, and landscape problems. Since the rotating speed of the rotating disk is not as high as that of wind power generation wings, there is little possibility of causing damage due to centrifugal force and collision death of marine animals.

また本回転盤を水面付近に設置すれば海流、潮流のみならず水面付近の波浪からもエネルギーを吸収することが出来る。しかも吸収量は後述のように、相乗効果により海流、潮流のみからエネルギーを吸収した量と波浪のみからエネルギーを吸収した量を加算した以上のエネルギーを生み出すことが出来る。 If this rotating disk is installed near the water surface, energy can be absorbed not only from ocean currents and tidal currents but also from waves near the water surface. Moreover, as will be described later, the amount of absorption can generate more energy than the sum of the amount of energy absorbed from only ocean currents and tidal currents and the amount of energy absorbed only from waves.

波浪からのエネルギーによる発電方式について、本発明者の発明である特許文献1、特開2011−117397(以下特許文献と称する)があるが、
特許文献の方式では、受流翼が垂直方向ではなく、本発明による水平方向の流れである海流、潮流エネルギーの吸収は出来ない。または効率が悪い。
また特許文献の方式では海流、潮流エネルギーと波浪エネルギーとの相乗効果が得られない。
Regarding power generation methods using energy from waves, there are Patent Document 1 and Japanese Patent Application Laid-Open No. 2011-117397 (hereinafter referred to as Patent Documents) which are the inventors' invention.
In the method of the patent document, the receiving wing is not in the vertical direction, and it is not possible to absorb the ocean current and tidal current energy which are horizontal flows according to the present invention. Or inefficient.
In addition, the method disclosed in the patent document cannot provide a synergistic effect between ocean current, tidal current energy and wave energy.

これに対して、本発明においては、受流翼は垂直方向に設置されており、それにより水平方向の流れである海流、潮流からのエネルギーを吸収できる。
また本発明の形状においては、受流翼に海流、潮流と波浪の運動が同時に同一場所に加わるので、エネルギーは受流翼に相加された流速の3乗に比例する形で加わり、各運動が個別に相加された量以上の効果があり、海流、潮流運動と波浪運動との相乗効果が得られる。
On the other hand, in the present invention, the receiving vanes are installed in the vertical direction, and thereby can absorb energy from ocean currents and tidal currents that are horizontal flows.
Further, in the shape of the present invention, since the ocean current, tidal current and wave motion are simultaneously applied to the receiving blade at the same place, energy is added in a form proportional to the cube of the flow velocity added to the receiving blade. There is an effect more than the amount added individually, and the synergistic effect of ocean current, tidal current and wave motion is obtained.

図1は実施形体を示す全体図である。FIG. 1 is an overall view showing an embodiment. 図2は実施形体を示す拡大図である。側面図である。FIG. 2 is an enlarged view showing the embodiment. It is a side view. 図3は実施形体の回転盤の一部の拡大図である。更に拡大図上である。FIG. 3 is an enlarged view of a part of the rotating disk of the embodiment. Furthermore, it is on an enlarged view. 図4は実施形態の上面図である。FIG. 4 is a top view of the embodiment. 図5は実施形体の側面図である。FIG. 5 is a side view of the embodiment. 図6は実施形態の受流翼の外観図である。FIG. 6 is an external view of the receiving vane of the embodiment. 図7は受流翼のピッチ変化を示す説明図である。FIG. 7 is an explanatory view showing the pitch change of the receiving blade. 図8は受流翼にかかる力のベクトルを示す説明図である。FIG. 8 is an explanatory diagram showing a force vector applied to the receiving blade. 図9は数値検討を示すための説明図である。FIG. 9 is an explanatory diagram for showing numerical examination. 図10は受流翼にかかる力のベクトルを示す説明図である。FIG. 10 is an explanatory diagram showing a force vector applied to the receiving blade. 図11は受流翼のピッチ変化を示す説明図である。FIG. 11 is an explanatory view showing a pitch change of the receiving blade. 図12は実施形体のピッチ変化を示す説明図である。FIG. 12 is an explanatory view showing a pitch change of the embodiment.

前記課題を解決するための手段で説明した面の向きが垂直方向の多数の受流翼を装備した回転盤を水面付近の水平の方向に設置し、または浮揚繋留させ、エネルギー源である海流、潮流運動から推進力を得て回転させ、この回転からエネルギーを吸収する実施例は以下の通りである。 A rotating disk equipped with a number of receiving wings whose vertical direction is the vertical direction described in the means for solving the above problems is installed in a horizontal direction near the water surface, or is levitated and tethered to the ocean current as an energy source, An example in which a propulsive force is obtained from the tidal current and rotated to absorb energy from the rotation is as follows.

図1は実施例1の実施形体を示す全体図である。図1において全体構造は水面付近に水平方向に設置された海流、潮流の運動により反対方向に回転する2つの回転盤11,12を有し、各回転盤には多数の受流翼3が取りつけられており、各翼3は海流、潮流の水流により推進力を得て回転盤を回転させる。回転盤の軸構造5は支持構造2に支えられている。 FIG. 1 is an overall view showing an embodiment of the first embodiment. In FIG. 1, the entire structure has two rotating discs 11 and 12 that rotate in opposite directions due to the movement of ocean currents and tidal currents installed in the horizontal direction near the water surface, and a large number of receiving vanes 3 are attached to each rotating disc. Each wing 3 obtains a propulsive force by the ocean current and tidal current and rotates the rotating disk. The shaft structure 5 of the rotating disk is supported by the support structure 2.

支持構造2はアンカー1および鎖13で海底または陸地に繋留されている。回転盤および支持構造は海流、潮流の流れにより下流方向に向かって力を受けるが、アンカー1および鎖13により押し流されることなく定位置にとどまる。これにより回転盤は流れに沿った水平方向の流圧を受け、後述のようにこの流圧力が回転盤を回転させる。 The support structure 2 is anchored to the seabed or land with anchors 1 and chains 13. The turntable and the support structure are subjected to a force in the downstream direction by the ocean current and tidal current, but remain in place without being swept away by the anchor 1 and the chain 13. As a result, the rotating disk receives a horizontal flow pressure along the flow, and this flow pressure rotates the rotating disk as will be described later.

2つの回転盤は海流、潮流の力を受けて反対方向に回転することにより各々の反作用である反対方向の力のモーメントが生ずるが、各力のモーメントは軸構造5を通じて支持構造2に伝わり、各回転盤が受ける回転モーメントは相殺され、支持構造自身が回転することはなく、安定した発電作用を支える。 The two rotating disks receive the forces of ocean currents and tidal currents and rotate in opposite directions to generate counter-forces of opposite forces, but the moments of each force are transmitted to the support structure 2 through the shaft structure 5, The rotational moment received by each turntable is canceled out, and the support structure itself does not rotate and supports a stable power generation operation.

図2は図1の全体図の拡大図である。軸構造5にはローター51とステーター52があり、ローターは回転盤と連結されており、回転盤により駆動され回転する。ステーターは支持構造2に固定され回転をせず、安定した発電作用を支える。支持構造2は鎖13を経由して海底または陸地に繋留される。鎖8には浮力を持ち海面に位置するブイ14がつながれており、鎖の重力または繋留の下方向の力で全体の設備が沈められたり傾くことを防止する。 FIG. 2 is an enlarged view of the overall view of FIG. The shaft structure 5 includes a rotor 51 and a stator 52. The rotor is connected to a rotating disk and is driven to rotate by the rotating disk. The stator is fixed to the support structure 2 and does not rotate, and supports a stable power generation operation. The support structure 2 is tethered to the seabed or land via a chain 13. The chain 8 is connected to a buoy 14 which has buoyancy and is located on the sea surface, and prevents the entire equipment from being sunk or tilted by the gravity of the chain or the downward force of the tether.

軸構造5には増速機、発電機が内蔵されており、回転盤の回転により駆動されて、発電が行われる。 The shaft structure 5 includes a speed increaser and a generator, and is driven by the rotation of the rotating disk to generate power.

また支持構造は浮力を持ち、この浮力は支持構造内部の空気を出し入れすることにより、適正な量に調整できる。これにより回転盤は海流、潮流エネルギー吸収に最適な上下位置に調整される。また建設時、保守時には作業をしやすい高さに上げられる。 The support structure has buoyancy, and this buoyancy can be adjusted to an appropriate amount by taking in and out air inside the support structure. As a result, the turntable is adjusted to the optimum vertical position for absorbing the ocean current and tidal current energy. It can also be raised to a height that is easy to work during construction and maintenance.

また暴風時に過度の風や波浪があるときにはその影響の少ない深度まで下げられ、破壊されることを防止する。 Also, when there are excessive winds and waves during a storm, it is lowered to a depth that has less influence to prevent it from being destroyed.

また建設時等で別の場所から牽引される場合等には、牽引されやすい高さに調整される。 Further, when the vehicle is towed from another place at the time of construction or the like, the height is adjusted to be easily pulled.

エネルギー採取方法として、発電機のかわりに高圧流体発生ポンプを駆動して、ここで発生した高圧流体をエネルギー源として利用することも可能である。 As an energy collecting method, it is possible to drive a high-pressure fluid generating pump instead of the generator and use the high-pressure fluid generated here as an energy source.

図3は回転盤の一部の拡大図である。回転盤にはフレーム8に装備された受流翼3があり、海流、潮流からの流圧を受け、これが回転駆動力となって回転盤を回転させる。 FIG. 3 is an enlarged view of a part of the rotating disk. The rotating disk has a receiving vane 3 mounted on the frame 8 and receives the flow pressure from the ocean current and tidal current, and this serves as a rotational driving force to rotate the rotating disk.

図4は本実施形体を示す上面図である。装置全体はアンカー1および鎖13で海底または陸地に繋留され、海流、潮流からの流圧で押し流されるのを防止し、また流圧が受流翼に加えられるようにする。 FIG. 4 is a top view showing this embodiment. The entire device is anchored to the seabed or land with anchors 1 and chains 13 to prevent being swept away by current pressure from the ocean current, tidal current, and to allow the fluid pressure to be applied to the receiving wing.

図5は本実施形体を示す側面図である。図に示されるように、回転盤11,12および各受流翼は水面6直下に位置し、海流、潮流の運動による流圧を受ける。全体構造は浮体型であり、アンカー1および鎖により海底9に繋留されている。アンカーにかかる力が大きい場合には、アンカーは海底に繋留構造物を設置するか陸上に設置された繋留構造物に固定される。鎖の代わりに大きな引張強度を持つ鋼製ワイアを使用しても良い。 FIG. 5 is a side view showing the present embodiment. As shown in the figure, the rotating disks 11 and 12 and the receiving blades are located immediately below the water surface 6 and receive a flow pressure due to the movement of ocean currents and tidal currents. The whole structure is a floating type, and is anchored to the seabed 9 by anchors 1 and chains. When the force applied to the anchor is large, the anchor is fixed to the anchoring structure installed on the seabed or on the land. A steel wire having a large tensile strength may be used instead of the chain.

またこの構造により、支持構造は海底7に固定される必要がなく、浮体型でよく、構造の簡単化、沖合での設置が可能となる。 Also, with this structure, the support structure does not need to be fixed to the seabed 7 and may be a floating body, which simplifies the structure and enables installation offshore.

水深が浅く工事が簡単であり、回転盤が単独の簡単な構造が望ましい場合には、回転盤の固定軸を海底に固定する方式(着底式)でもよい。この場合には回転盤が回転する場合の反作用としての力のモーメントは海底に固定された固定軸で支持されるので、図1にしめす支持構造2は不要になる。また回転盤は単独でよく、全体の構造は簡単になる。 When the water depth is shallow and the construction is simple and a simple structure with a single rotating disk is desirable, a method of fixing the fixed axis of the rotating disk to the seabed (bottomed) may be used. In this case, since the moment of force as a reaction when the rotating disk rotates is supported by a fixed shaft fixed to the seabed, the support structure 2 shown in FIG. 1 is unnecessary. Moreover, the rotating disk may be independent and the whole structure becomes simple.

発電された電力または発生された高圧流体は、海底に沿ってまたは海中に設置された送電線またはパイプにより陸上に送られ利用される。この送電線またはパイプは上記の鎖と束ねられて強度を保つ方法も可能である。水深が深くアンカーの設置が困難な場合は送電線またはパイプとともに陸上または水深の浅い場所まで延長し固定される。 The generated electric power or generated high-pressure fluid is sent to land for use by transmission lines or pipes installed along the seabed or in the sea. This transmission line or pipe can be bundled with the above-mentioned chain to keep the strength. If the depth of water is deep and it is difficult to install the anchor, it will be fixed with the transmission line or pipe to the land or to a shallow depth.

さらに設置場所が沖合にあり送電線またはパイプを陸上に延長することが困難な場合には、発電された電力で大型蓄電器を充電しこれを船舶等で利用地に運搬する方法もある。または発電された電力で水素等のエネルギーを蓄積できる物質を発生させてこれを船舶等で利用地に運搬する方法もある。 Furthermore, when the installation site is offshore and it is difficult to extend the transmission line or pipe to the land, there is also a method of charging a large-sized battery with the generated power and transporting it to a use site by a ship or the like. Alternatively, there is a method in which a substance that can store energy such as hydrogen is generated by the generated electric power and transported to a place of use by a ship or the like.

図6は1枚の受流翼3の実施形態例の外観を示したものである。受流翼3には回転軸31があり、図3のフレーム8に連結されている。受流翼のピッチはこの回転軸を中心に変化する。回転軸は回転方向に弾性を持ち、海流、潮流の流圧が受流翼に加わることにより、受流翼の角度すなわちピッチが変化する。すなわち受流翼のピッチは受動的に変化する。 FIG. 6 shows the external appearance of an embodiment of the single receiving blade 3. The receiving blade 3 has a rotating shaft 31 and is connected to the frame 8 of FIG. The pitch of the receiving blade changes around this rotation axis. The rotating shaft has elasticity in the direction of rotation, and the angle of the receiving blade, that is, the pitch, changes as the current pressure of the ocean current and tidal current is applied to the receiving blade. That is, the pitch of the receiving vanes changes passively.

図7は海流、潮流の運動による受流翼の変形をしめす説明図である。波の水流が図の下から上に向かう場合は、受流翼は上に向かう方向に力を受け、弾性を持つ受流翼は上方向に変形し、水流により図の左方向に力を受ける。波の水流方向が上から下に向かう場合は、弾性部分は下方向に変形し、水流により図の左方向に力を受ける。すなわち波の水流の方向に係らず、各受流翼は図の左方向に推進力を受け、左方向に走行する。実際の受流翼は回転盤に同心円状に配置されているので、受流翼が受ける推進力は回転盤を同一方向に回転させる方向に働く。 FIG. 7 is an explanatory view showing the deformation of the receiving wing due to the movement of the ocean current and tidal current. When wave water flows from the bottom to the top of the figure, the receiving blade receives force in the upward direction, the elastic receiving blade deforms upward, and the water flow receives force in the left direction in the figure. . When the water current direction of the wave is from the top to the bottom, the elastic portion is deformed downward and receives a force in the left direction of the figure by the water flow. That is, regardless of the direction of wave water flow, each receiving blade receives a driving force in the left direction of the figure and travels in the left direction. Since the actual receiving vanes are arranged concentrically on the rotating disk, the propulsive force received by the receiving vanes acts in the direction of rotating the rotating disk in the same direction.

図8は波海流、潮流、波浪の水流により受流翼が受ける力をベクトルとして示したものである。受流翼は水流により、翼面と垂直の方向に力Foを受ける。Foは回転盤と垂直の方向Fbと水平の方向Faに分解される。Faは水流の方向に係らず図の左方向に向き、回転盤を同一方向に推進する力となる。 FIG. 8 shows, as a vector, the force that the receiving wing receives from the wave current, tidal current, and wave current. The receiving wing receives a force Fo in a direction perpendicular to the wing surface due to water flow. Fo is decomposed into a direction Fb perpendicular to the rotating disk and a direction Fa horizontal. Fa is directed to the left in the figure regardless of the direction of water flow, and is the force that propels the rotating disk in the same direction.

以下に数値的検討を示す。 The numerical examination is shown below.

図9は概略的な定量的説明を行うためのベクトル図である。図において水平線は回転盤を表し、斜線は受流翼を表す。   FIG. 9 is a vector diagram for a rough quantitative explanation. In the figure, the horizontal line represents the rotating disk, and the diagonal line represents the receiving blade.

図において各パラメータおよび変数を以下のように定める。
Fo : 波浪により受流翼にかかる力
Fa: 受流翼にかかる水平力(走行推進力)
Fb: 受流翼にかかる垂直力(非走行力)
Vc: 波浪運動の垂直成分速度
Va: 受流翼走行速度
Vd: 受流翼走行による波浪速度等価減速分
So: 受流翼面積
θ: 受流翼のピッチ角度
ρ: 水の重量密度
P: 受流翼走行による利用可能な時間当たりのエネルギー(発電量)
In the figure, each parameter and variable are defined as follows.
Fo: Force applied to the receiving wing by waves
Fa: Horizontal force on the receiving wing (traveling propulsion force)
Fb: Normal force applied to the receiving blade (non-running force)
Vc: Vertical component velocity of wave motion
Va: Receiving blade travel speed
Vd: Wave speed equivalent deceleration by receiving blade travel
So: receiving blade area θ: pitch angle of receiving blade ρ: weight density of water
P: Energy available per hour (power generation)

まず波浪により受流翼にかかる力Foは、
Fo = ρSo (Vc − Vd) 2 = ρSo (Vc − Va sinθ)2 ---------- (1)
となる。
ここで受流翼走行による波浪速度等価減速分 Vdは、
Vd =
Va sinθ
--------- (2)
で表される。
First, the force Fo applied to the receiving wing by waves is
Fo = ρSo (Vc − Vd) 2 = ρSo (Vc − Va sinθ) 2 ---------- (1)
It becomes.
Here, the wave velocity equivalent deceleration Vd due to running of the receiving blade is
Vd =
Va sinθ
--------- (2)
It is represented by

受流翼がうける走行推進力Faは、
Fa = Fo sinθ =ρSo (Vc − Va sinθ)2 sinθ -----------
(3)
受流翼に発生する利用可能な時間あたりのエネルギーPは、
P =Va Fa = ρSo Va (Vc −Va sinθ)2 sinθ ----------- (4)
となる。
The driving force Fa received by the receiving blade is
Fa = Fo sinθ = ρSo (Vc − Va sinθ) 2 sinθ -----------
(3)
The available energy per hour P generated in the receiving blade is
P = Va Fa = ρSo Va (Vc −Va sinθ) 2 sinθ ----------- (4)
It becomes.

ここで k を波浪速度等価減速係数として
k
= Vd / Vc = Va sinθ /Vc -------------------------- (5)
とすると、
P = ρSo Vc3(1− k)2 k ---------- (6)
となる。
Where k is the wave velocity equivalent deceleration coefficient
k
= Vd / Vc = Va sinθ / Vc -------------------------- (5)
Then,
P = ρSo Vc 3 (1− k) 2 k ---------- (6)
It becomes.

Pをkで微分してPの最大値を求めると、Pは k = 1/3の時最大となる。
Pすなわち発電量の最大値をPmax、このときの(1−k)2kの値を効率係数μaとすると、μa = 0.148
-------------- (7)
となり
Pmax = ρSo Vc3 (1−k)2k =ρμa So Vc3 =
0.148ρSo Vc3 ------------------( 8)
となる。
Differentiating P by k to find the maximum value of P, P is maximum when k = 1/3.
P, that is, the maximum value of power generation is Pmax, and the value of (1−k) 2 k is μa = 0.148
-------------- (7)
Next
Pmax = ρSo Vc 3 (1−k) 2 k = ρμa So Vc 3 =
0.148ρSo Vc 3 ------------------ (8)
It becomes.

具体的な数値例は以下の通りである。
海流、潮流の流速Vcを2.5m/sとし、回転盤の外径Raを100m、同心円上に配置された受流翼段数を4 内径Rbを70m、受流翼の高さを5mとすると、受流翼総面積Saは
Sa = 2πh(Ra/2)(1+0.9+0.8+0.7)
=5,341m2 ------------------( 9)

海流、潮流が一方向から来るとして、波の受ける受流翼の実効面積SoはSaの半分とすると、
So = Sa / 2 = 2,670m2 --------- (10)
となる。
Specific numerical examples are as follows.
When the ocean current and tidal current velocity Vc is 2.5 m / s, the outer diameter Ra of the rotating disk is 100 m, the number of receiving blade stages arranged concentrically is 4 inner diameter Rb is 70 m, and the height of the receiving blade is 5 m. Receiving blade total area Sa
Sa = 2πh (Ra / 2) (1 + 0.9 + 0.8 + 0.7)
= 5,341m 2 ------------------ (9)

Assuming that the ocean current and tidal current come from one direction, the effective area So of the receiving wing that the wave receives is half of Sa,
So = Sa / 2 = 2,670m 2 --------- (10)
It becomes.

式(7)で示すように、受流翼で海流、潮流のエネルギーを吸収する最大効率μaは0.148である。
その他の損失を考えた発電効率μgとし
μg = 0.4
----------(11)
とし、海水の重量密度を、1,025 Kg /
m3 とすると、最大発電量Pmaxは、
Pmax = ρSo Vc3 (1−k)2k =ρμgμa So Vc3 = 0.044ρSo Vc3=1,882KW ----------(12)

となる。
As shown in Equation (7), the maximum efficiency μa for absorbing the energy of the ocean current and tidal current with the receiving wing is 0.148.
Power generation efficiency μg considering other losses
μg = 0.4
---------- (11)
And the weight density of seawater is 1,025 kg /
Assuming m 3 , the maximum power generation Pmax is
Pmax = ρSo Vc 3 (1−k) 2 k = ρμgμa So Vc 3 = 0.044ρSo Vc 3 = 1,882KW ---------- (12)

It becomes.

回転翼が2つの場合には、発電量はその2倍の3,764KW、回転翼がN個の場合はN倍となる。 When there are two rotor blades, the power generation amount is 3,764KW, twice that amount, and when there are N rotor blades, it is N times.

実際の発電量は、翼の形状、複雑な波の形や周期、季節変化、異なる波の重なり合い、具体的な発電効率等、多くの複雑な要因があり、正確に推定するのは容易ではないが、上記の値は概略の推定例となる。   Actual power generation has many complicated factors such as wing shape, complex wave shape and period, seasonal changes, overlapping of different waves, and specific power generation efficiency, and it is not easy to estimate accurately. However, the above value is a rough estimation example.

実際の海洋においては、海流、潮流とともに波浪運動が存在する。受流翼は海流、潮流運動とともに波浪運動も受ける。受流翼はこの波浪エネルギーも同時に複合的に吸収する。
吸収するエネルギーは受流翼にあたる海水速度の3乗に比例するので、吸収するエネルギーは単に直線的の相加されるのではなく、それ以上の値で相加され、相乗効果がある。
In the actual ocean, wave motions exist along with ocean currents and tidal currents. The receiving wing is subject to wave motion as well as ocean current and tidal current motion. The receiving blade also absorbs this wave energy in a complex manner.
Since the energy to be absorbed is proportional to the cube of the seawater velocity corresponding to the receiving blade, the energy to be absorbed is not simply added in a linear manner, but is added at a value higher than that and has a synergistic effect.

海流、潮流の流速をa、波浪の流速の振幅をbとすると、相加された流速Veは、
Ve = a + bsin( 2πt/T + θ) ----------(13)
となる。ここでTは波の周期、θは定数でありここではゼロとする。
If the current velocity of ocean current and tidal current is a and the amplitude of wave velocity is b, the added velocity Ve is
Ve = a + bsin (2πt / T + θ) ---------- (13)
It becomes. Here, T is the wave period, and θ is a constant, which is zero here.

吸収エネルギーはVeの3乗に比例するので、波浪が相加された場合と相加されない場合の吸収エネルギーの比をμcは、

Figure 2013036365
海流、潮流の流速aを2.5m/s、波浪の流速の振幅bを2.0m/sとすると、μcは2.03となる。
すなわち波浪が加わった場合には、加わらない場合の2.03倍もの発電量が発生する。相乗効果は大きい。 Since the absorbed energy is proportional to the cube of Ve, the ratio of the absorbed energy when the wave is added and not added is μc,
Figure 2013036365
If the current velocity a of ocean current and tidal current is 2.5 m / s and the amplitude b of wave current velocity is 2.0 m / s, μc is 2.03.
In other words, when waves are added, the amount of power generation is 2.03 times as much as when no waves are added. The synergistic effect is great.

もし海流、潮流と波浪が別の所に当たり相乗効果がなく、海流、潮流による発電と波浪による発電が単純に加算されたとすると、波浪が相加された場合と相加されない場合の吸収エネルギーの比μsは、

Figure 2013036365
海流、潮流の流速aを2.5m/s、波浪の流速の振幅bを2.0m/sとすると、μsは1.13となる。
すなわち海流、潮流と波浪が別の所に当たり、相乗効果がない場合は、吸収エネルギー比μsは1.13(13%増)に過ぎず、前記の波浪が相乗効果として加わった場合のμcの2.03(103%増)が如何に大きいかが分かる。 If the ocean currents, tidal currents and waves are in different locations and there is no synergistic effect, and the power generation by ocean currents and tidal currents and the power generation by waves are simply added, the ratio of the absorbed energy when the waves are added and not added μs is
Figure 2013036365
If the current flow velocity a of ocean current and tidal current is 2.5 m / s and the amplitude b of wave current velocity is 2.0 m / s, μs is 1.13.
In other words, when the ocean current, tidal current and waves are in different places and there is no synergistic effect, the absorbed energy ratio μs is only 1.13 (13% increase), and 2.03 (103 of μc when the waves are added as a synergistic effect. You can see how big (% increase) is.

上記の数値例では相乗効果を考慮したμcと考慮しないμsの比は2.1であり、海流、潮流と波浪を組み合わせた場合の相乗効果は2倍以上である。
現実の海上環境では海流、潮流と波浪の運動には上記の相乗効果が発生するので、海流、潮流と波浪を組み合わせた発電の効果は極めて大きいと言える。
In the above numerical example, the ratio of μs taking into account the synergistic effect and μs not taking into consideration is 2.1, and the synergistic effect when the ocean current, tidal current and wave are combined is more than twice.
In the actual marine environment, the above-mentioned synergistic effect occurs in the movement of ocean currents, tidal currents and waves, so it can be said that the effect of power generation combining ocean currents, tidal currents and waves is extremely large.

本海流、潮流発電方式は、設備全体として海洋上に水平方向に設置されるので、利用対象として海流、潮流、波浪を含めることができ、総合的な相乗効果を持つ効率の良い海洋エネルギー発電方式として使うことが出来る。 This ocean current and tidal current power generation method is installed horizontally on the ocean as a whole facility, so it can include ocean currents, tidal currents, and waves, and it is an efficient ocean energy power generation method that has a comprehensive synergistic effect. Can be used as

受流翼のピッチの変化には3つの形態がある。いずれの形態でも受流翼は海水の動きの方向にかかわらず同一方向の推進力を受ける。
第一の受流翼ピッチの形態は、上記実施の形態例および図7で説明した、海流、潮流の流圧を受けて特にピッチ角度を制御しなくてもピッチ角が受動的に変化する受動型可変ピッチ受流翼である。受流翼のピッチすなわち角度は、流体運動の圧力を受けて変形する。
There are three forms of changes in the pitch of the receiving blade. In any form, the receiving blade receives the propulsive force in the same direction regardless of the direction of movement of the seawater.
The form of the first receiving blade pitch is passive in which the pitch angle is passively changed even if the pitch angle is not particularly controlled in response to the sea current and tidal current pressure described in the above embodiment and FIG. This is a variable pitch receiving blade. The pitch or angle of the receiving blade is deformed under the pressure of fluid motion.

このためには受流翼材料に弾性を持たせるか受流翼を支える軸にばねを仕込むなりして弾性を持たせる。流体の当たる速度が大きく流体圧力が大きい場合にはピッチ(角度)変化量が大きくなり、エネルギー吸収効率があがる。
ただし必要以上にピッチが大きくなると受流翼の受ける流圧が減少し逆にエネルギー吸収効率は下がる。すなわちピッチ角には、前記の式7で説明したように流体速度に対応した最適値がある。
For this purpose, the receiving blade material is made elastic or a spring is loaded on the shaft that supports the receiving blade to make it elastic. When the fluid contact speed is large and the fluid pressure is large, the amount of change in pitch (angle) increases, and the energy absorption efficiency increases.
However, if the pitch becomes larger than necessary, the flow pressure received by the receiving blades decreases, and conversely the energy absorption efficiency decreases. In other words, the pitch angle has an optimum value corresponding to the fluid velocity, as described in Equation 7 above.

この受動型可変ピッチ受流翼の利点は特にピッチ制御を行う必要がなく、構造が簡単になることであるが、それぞれの受流翼のピッチを最適値に近づけるように、弾性力を設定することが必要である。 The advantage of this passive variable pitch receiving blade is that there is no need to perform pitch control and the structure is simple, but the elastic force is set so that the pitch of each receiving blade is close to the optimum value. It is necessary.

第2の受流翼ピッチの形態はピッチが変化しない固定型ピッチである。図6の受流翼実施例において軸が弾力を持たず海流、潮流の動きがあってもピッチが変化しない場合には固定ピッチ型受流翼となる。 The form of the second receiving blade pitch is a fixed pitch in which the pitch does not change. In the embodiment of the receiving blade of FIG. 6, if the shaft does not have elasticity and the pitch does not change even when there is a sea current or tidal current movement, a fixed pitch type receiving blade is obtained.

受流翼の形状によってはピッチを変えなくても常に同方向の推進力が生ずる。これはウェールズタービンとも呼ばれるもので、風力発電でもダリウス型と称せられるものはこの原理を使っている。 Depending on the shape of the receiving vane, the propulsive force in the same direction is always generated without changing the pitch. This is also called a Welsh turbine, and what is called Darius type in wind power generation uses this principle.

固定ピッチ型受流翼を本発明の方式に適用すれば、ピッチを変える必要がないので受流翼を装備した回転盤全体の構造を強固に簡単にできる。ただし問題点としては、一般的にウェールズタービンはある程度の速度以上にならないと推進力が大きくならない。このために初期の起動時には何かしらの起動力を加えることが必用である。また一般的にはウェールズタービン型の翼は厚さが比較的大きく、回転時の抵抗が大きくなり、発電効率を減少させる可能性がある。 If a fixed pitch type receiving vane is applied to the method of the present invention, it is not necessary to change the pitch, so that the structure of the entire rotating disk equipped with the receiving vane can be strongly and simply. However, as a problem, generally, a Welsh turbine does not increase its propulsive force unless it exceeds a certain speed. For this reason, it is necessary to apply some kind of starting force at the time of initial startup. In general, a Welsh turbine-type blade is relatively thick and has a large resistance during rotation, which may reduce power generation efficiency.

図10は固定ピッチ型受流翼にかかる力のベクトル図を示すものである。
図10において左側の受流翼には図の下から上に向かう海流、潮流の動きが加わり、その結果揚力Foが生ずる。この揚力は受流翼に垂直の方向の力Fbと受流翼に沿った方向の力Faに分解できる。Faは受流翼を図の左に推進する力となる。
図10において右側の受流翼には図の上から下に向かう海流、潮流の動きが加わり、その結果揚力Foが生ずる。この揚力は受流翼に垂直の方向の力Fbと受流翼に沿った方向の力Faに分解できる。Faは受流翼を図の左に推進する力となる。
すなわち受流翼に加わる海流、潮流の方向にかかわらず受流翼は図の同じ左方向に推進する力を受け、回転盤を同方向に推進する。
FIG. 10 shows a vector diagram of the force applied to the fixed pitch type receiving blade.
In FIG. 10, the current receiving wing on the left side is subjected to the movement of ocean currents and tidal currents from the bottom to the top of the figure, resulting in lift Fo. This lift can be decomposed into a force Fb in the direction perpendicular to the receiving blade and a force Fa in the direction along the receiving blade. Fa is the force that propels the receiving wing to the left of the figure.
In FIG. 10, the current receiving wing on the right side is subjected to the movement of ocean currents and tidal currents from the top to the bottom of the figure, resulting in lift Fo. This lift can be decomposed into a force Fb in the direction perpendicular to the receiving blade and a force Fa in the direction along the receiving blade. Fa is the force that propels the receiving wing to the left of the figure.
In other words, regardless of the direction of the ocean current and tidal current applied to the receiving blade, the receiving blade receives the force propelled in the same left direction in the figure and propels the rotating disk in the same direction.

固定ピッチ型の受流翼を使う利点は構造が簡単であり、受流翼と回転盤は固定されるので、構造的な強度が保たれることである。問題点は前記のように十分な揚力が生ずるためには受流翼の走行速度がある程度大きいことが必要なことである。そのために回転盤が動き始める初期においては起動力が必要になることがある。 The advantage of using a fixed pitch type receiving blade is that the structure is simple and the receiving blade and the rotating disk are fixed, so that the structural strength is maintained. The problem is that the traveling speed of the receiving blade needs to be high to some extent in order to generate sufficient lift as described above. For this reason, an activation force may be required at an early stage when the rotating disk starts to move.

起動力を生じさせる方法の一つは、回転盤に装備される受流翼を、図8に示す可変ピッチ型の受流翼と図10に示す固定ピッチ型の受流翼の両方を組み合わせて装備する方法である。可変ピッチ型の受流翼は初期の起動力を必要とはしないので、起動の初期においては可変ピッチ型の受流翼が回転盤を駆動し、回転盤の回転速度すなわち受流翼の走行速度が上がるにつれて固定ピッチ型の駆動力が増大する。これにより固定ピッチ型受流翼の利点が保たれる。 One method for generating the starting force is to combine the receiving blades mounted on the rotating disk with the variable pitch type receiving blades shown in FIG. 8 and the fixed pitch type receiving blades shown in FIG. How to equip. Since the variable pitch type receiving blade does not require the initial starting force, the variable pitch type receiving blade drives the rotating disk at the initial stage of starting, and the rotating speed of the rotating disk, that is, the traveling speed of the receiving blade. As the speed increases, the fixed-pitch driving force increases. Thereby, the advantage of a fixed pitch type receiving blade is maintained.

動力を生じさせる他の方法のは、固定ピッチ型の受流翼の後方すなわち図10の受流翼の右後部に多少の弾力を持たせることである。弾力を持たせることにより受流翼は海流、潮流の動きを受けて、図8に示す形に類似して変形し、走行速度が小さくても駆動力を受け、起動を助ける。 Another method of generating power is to give some elasticity to the rear of the fixed pitch type receiving blade, that is, the right rear portion of the receiving blade in FIG. By providing elasticity, the receiving wing receives the movement of the ocean current and tidal current and is deformed in a manner similar to the shape shown in FIG.

第3の受流翼ピッチの形態は、受動的でも固定的でもなく、各受流翼にピッチ角制御機構を持たせて、能動的にピッチを制御する方法である。海流、潮流の方向がある時間一定である場合は、ピッチは必ずしも個々の区分で受動的に変化させる必要はなく、全体の海流、潮流の流れる方向によって、能動的にピッチ角を制御しても良い。すなわち個々の受流翼のピッチが海流、潮流の流れの流圧によって変化するのではなく、予め設定されたピッチ制御機構によりピッチ角度を能動的に変化させる。 The form of the third receiving blade pitch is neither passive nor fixed, and is a method of actively controlling the pitch by providing each receiving blade with a pitch angle control mechanism. If the direction of the ocean current and tidal current is constant for a certain period of time, the pitch does not necessarily have to be changed passively in each section. Even if the pitch angle is actively controlled according to the direction of the entire ocean current and tidal current, good. That is, the pitch of each receiving blade is not changed by the flow pressure of the ocean current and tidal current, but the pitch angle is actively changed by a preset pitch control mechanism.

流体の速度や方向がほぼ一定であれば、最適ピッチ角度は予め分かり、この値に合うようにピッチ角を制御することが出来る。ただし海流、潮流に適用する場合は、回転盤の回転位置によってピッチを制御する必要がある。 If the velocity and direction of the fluid are substantially constant, the optimum pitch angle is known in advance, and the pitch angle can be controlled to match this value. However, when applied to ocean currents and tidal currents, it is necessary to control the pitch according to the rotational position of the rotating disk.

能動的のピッチを制御する技術は航空機や船舶で広く使われており、技術としては一般的に確立している。 Active pitch control technology is widely used in aircraft and ships, and is generally established as a technology.

図11は海流、潮流の方向が一定である場合の、受流翼のピッチが能動的に制御された例を示す。図において海流、潮流は図の上から下の方向に向かって流れている。受流翼のピッチは全体の中の位置で図のような角度に制御される。この結果受流翼は海流、潮流の流れを受け、回転盤を反時計方向に駆動する。 FIG. 11 shows an example in which the pitch of the receiving blade is actively controlled when the direction of the ocean current and the tidal current is constant. In the figure, ocean currents and tidal currents flow from the top to the bottom of the figure. The pitch of the receiving blades is controlled to the angle shown in the figure at a position in the whole. As a result, the receiving blade receives the flow of ocean current and tidal current and drives the rotating disk counterclockwise.

能動的ピッチ制御受流翼の問題点は構造が複雑になること、および海流、潮流の流れの方向がある時間一定であることが必要なことである。また流れの方向は一定でない波浪を対象とした波浪発電には適用できない。 The problem with active pitch-controlled receiving blades is that the structure is complicated and that the direction of the ocean current and tidal current must be constant for a certain period of time. In addition, it cannot be applied to wave power generation for waves whose flow direction is not constant.

図12は陸地に近い海流、潮流の流速の速い場所で多数の回転盤を設置した例である。図において海洋20は陸地21に挟まれており、流速は大きい。複数の回転盤11は支持構造2で支えられている。支持構造2は両側の陸地21に固定されており潮流の流れに流されることはなく定位置にある。回転盤は海流、潮流および波浪の複合運動を受けて回転し発電する。 FIG. 12 shows an example in which a large number of turntables are installed in a place near the land where the ocean current and the tidal current are fast. In the figure, the ocean 20 is sandwiched between land 21 and the flow velocity is large. The plurality of turntables 11 are supported by the support structure 2. The support structure 2 is fixed to the land 21 on both sides and is not in a tidal flow and is in a fixed position. The rotating disk rotates and generates electricity under the combined movement of ocean currents, tidal currents and waves.

海上交通を妨げないためには、航路付近には回転盤を設置しないか、また支持構造を航行の妨げにならない水深まで下げる。
In order not to obstruct maritime traffic, do not install a turntable near the channel, or lower the support structure to a depth that does not hinder navigation.

本発明の海流、潮流発電方式は、大型で効率が良くコストも安い海流、潮流波浪の複合発電を実現でき、今後の自然エネルギーの利用およびそれに伴うCO2の削減、エネルギー資源偏在是正、新たな経済活動の創出等に大きな効果を発揮することができる。 The ocean current and tidal current power generation method of the present invention can realize a combined power generation of ocean currents and tidal waves that are large, efficient, and low in cost, use of natural energy in the future, and accompanying reduction of CO2, correction of uneven distribution of energy resources, new economy It can be very effective in creating activities.

1 アンカー
2 支持構造
3 受流翼
5 軸構造
6 水面
7 海底
8 フレーム
11 回転盤
12 回転盤
13 鎖
14 ブイ
31 受流翼軸
51 ローター
52 ステーター


DESCRIPTION OF SYMBOLS 1 Anchor 2 Support structure 3 Receiving blade 5 Shaft structure 6 Water surface 7 Seabed 8 Frame 11 Rotating disk 12 Rotating disk 13 Chain 14 Buoy 31 Receiving wing axis 51 Rotor 52 Stator


Claims (2)

面の向きが垂直方向の多数の受動可変ピッチまたは多数の揚力発生型の固定ピッチまたは多数の能動可変ピッチの受流翼を装備した回転盤を水面付近の水平の方向に着底型設置または浮体繋留設置し、エネルギー源である海流、潮流運動から同一方向の推進力を得て回転させ、この回転からエネルギーを吸収し発電することを特徴とする海洋エネルギー発電方式。
A rotating board equipped with multiple passive variable pitch or multiple lift generating fixed pitch or multiple active variable pitch receiving vanes whose surface orientation is vertical, is a bottomed installation or floating body in the horizontal direction near the water surface A marine energy power generation system characterized in that it is tethered and rotated by obtaining a propulsion force in the same direction from the ocean currents and tidal currents that are energy sources, and absorbing energy from this rotation.
回転盤を水面付近の波浪運動を受けやすい位置に設置し海流、潮流運動とともに波浪運動も受けるようにした、請求項1に示す海洋エネルギー発電方式。




2. The ocean energy power generation system according to claim 1, wherein the turntable is installed at a position where the wave motion near the surface of the water is easily received to receive the wave motion along with the ocean current and the tidal current motion.




JP2011171413A 2011-08-04 2011-08-04 Ocean energy power generation system Withdrawn JP2013036365A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2011171413A JP2013036365A (en) 2011-08-04 2011-08-04 Ocean energy power generation system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2011171413A JP2013036365A (en) 2011-08-04 2011-08-04 Ocean energy power generation system

Publications (1)

Publication Number Publication Date
JP2013036365A true JP2013036365A (en) 2013-02-21

Family

ID=47886206

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2011171413A Withdrawn JP2013036365A (en) 2011-08-04 2011-08-04 Ocean energy power generation system

Country Status (1)

Country Link
JP (1) JP2013036365A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20180137962A (en) * 2017-06-20 2018-12-28 최준서 Sonar for detecting submarines

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20180137962A (en) * 2017-06-20 2018-12-28 최준서 Sonar for detecting submarines
KR102011196B1 (en) * 2017-06-20 2019-08-14 최준서 Sonar for detecting submarines

Similar Documents

Publication Publication Date Title
JP6117105B2 (en) Wind energy utilization equipment and method
US8421260B2 (en) Hydrokinetic turbine for low velocity currents
US8362631B2 (en) Marine energy hybrid
JP6014591B2 (en) System and method for generating electricity from a flowing stream of fluid
US20110115231A1 (en) Hydrokinetic energy conversion system
US20120187693A1 (en) Hydrokinetic energy transfer device and method
US20080012345A1 (en) Tethered propgen
KR101242064B1 (en) Apparatus for Reducing Drag of Offshore Wind Power System
EP2545276B1 (en) Wind power system
US20090236858A1 (en) Vertical turbine for water or wind power generation
GB2486911A (en) Generating energy from a current flowing in a body of water
US9777709B2 (en) Translating foil system for harvesting kinetic energy from wind and flowing water
CN103930670A (en) Systems and methods for improved water rotors
WO2015142737A1 (en) Floating tower frame for ocean current turbine system
CN204527560U (en) A kind of semisubmersible wave energy-energy and wind energy integrative utilizes device
JP2013002399A (en) Ocean wind power generation wind turbine unflowing by wind even without mooring to sea bottom, by using a part of wind power for windward propulsion
AU2015291050B2 (en) Wave energy converter
Tsao et al. Marine current power with cross-stream active mooring: Part I
KR20090097089A (en) Flow rate generator
CN102705147A (en) Wave energy conversion device
JP3530872B2 (en) Hydro energy converter
JP2021533320A (en) Wind turbines, heat pumps, energy conservation, and heat transfer systems and methods
JP5190716B2 (en) Wave power generation method
JP2013019387A (en) Water current power generation system
KR20070026780A (en) Underwater power generation system

Legal Events

Date Code Title Description
A300 Withdrawal of application because of no request for examination

Free format text: JAPANESE INTERMEDIATE CODE: A300

Effective date: 20141007