WO2015190297A1 - Wave-activated power generation system - Google Patents
Wave-activated power generation system Download PDFInfo
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- WO2015190297A1 WO2015190297A1 PCT/JP2015/065343 JP2015065343W WO2015190297A1 WO 2015190297 A1 WO2015190297 A1 WO 2015190297A1 JP 2015065343 W JP2015065343 W JP 2015065343W WO 2015190297 A1 WO2015190297 A1 WO 2015190297A1
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- WIPO (PCT)
- Prior art keywords
- power generation
- wave
- generation system
- water
- wave power
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- 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.)
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Classifications
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- E—FIXED CONSTRUCTIONS
- E02—HYDRAULIC ENGINEERING; FOUNDATIONS; SOIL SHIFTING
- E02B—HYDRAULIC ENGINEERING
- E02B3/00—Engineering works in connection with control or use of streams, rivers, coasts, or other marine sites; Sealings or joints for engineering works in general
- E02B3/04—Structures or apparatus for, or methods of, protecting banks, coasts, or harbours
- E02B3/06—Moles; Piers; Quays; Quay walls; Groynes; Breakwaters ; Wave dissipating walls; Quay equipment
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- E—FIXED CONSTRUCTIONS
- E02—HYDRAULIC ENGINEERING; FOUNDATIONS; SOIL SHIFTING
- E02B—HYDRAULIC ENGINEERING
- E02B9/00—Water-power plants; Layout, construction or equipment, methods of, or apparatus for, making same
- E02B9/08—Tide or wave power plants
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F03—MACHINES OR ENGINES FOR LIQUIDS; WIND, SPRING, OR WEIGHT MOTORS; PRODUCING MECHANICAL POWER OR A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
- F03B—MACHINES OR ENGINES FOR LIQUIDS
- F03B13/00—Adaptations of machines or engines for special use; Combinations of machines or engines with driving or driven apparatus; Power stations or aggregates
- F03B13/12—Adaptations of machines or engines for special use; Combinations of machines or engines with driving or driven apparatus; Power stations or aggregates characterised by using wave or tide energy
- F03B13/14—Adaptations of machines or engines for special use; Combinations of machines or engines with driving or driven apparatus; Power stations or aggregates characterised by using wave or tide energy using wave energy
- F03B13/22—Adaptations of machines or engines for special use; Combinations of machines or engines with driving or driven apparatus; Power stations or aggregates characterised by using wave or tide energy using wave energy using the flow of water resulting from wave movements to drive a motor or turbine
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- Y—GENERAL 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
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02A—TECHNOLOGIES FOR ADAPTATION TO CLIMATE CHANGE
- Y02A10/00—TECHNOLOGIES FOR ADAPTATION TO CLIMATE CHANGE at coastal zones; at river basins
- Y02A10/11—Hard structures, e.g. dams, dykes or breakwaters
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- Y—GENERAL 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
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E10/00—Energy generation through renewable energy sources
- Y02E10/30—Energy from the sea, e.g. using wave energy or salinity gradient
Definitions
- the present invention relates to a wave power generation system that dissipates wave energy and generates power from the wave energy.
- wave power generation uses wave power generated in the sea covering 70% of the earth's surface, and has attracted attention as a powerful energy source.
- Patent Document 1 discloses a wave power generation system in which a water turbine is installed in a recreation water chamber of a breakwater that is installed in a relatively large amount in a harbor sea area. That is, the wave power generation system disclosed in Patent Document 1 can be easily installed because it uses the existing port infrastructure, and can further reduce the cost required for adding a power generation device and a power transmission facility.
- Patent Document 1 a breakwater having an impermeable wall on the shore side and a permeable front wall having a vertical slit on the offshore side is used.
- This type of breakwater ensures the calmness of the shore by reflecting the waves on the impervious wall and dissipates the energy of the waves by the vortices generated in the vicinity of the vertical slit on the front wall.
- the reflectance of the wave in an impermeable wall can be reduced and not only the shore side but the calmness of the offshore side through which a ship etc. pass can be ensured.
- the present invention aims to provide a wave power generation system capable of improving power generation efficiency while maintaining quietness.
- a wave power generation system is a wave power generation system that is used together with a breakwater to dissipate wave energy and generate electric power from the wave energy.
- the breakwater is a breakwater that is installed in water and has an impermeable wall, but does not have a permeable front wall on the offshore side of the impermeable wall.
- the rotating body row includes a plurality of rotating bodies arranged on the offshore side of the impermeable wall along a direction in which the impermeable wall extends in a plan view. The generator converts rotational energy of the plurality of rotating bodies into electric power.
- a transmissive front wall is not installed, but a rotating body row is installed instead.
- the energy of the wave that has been dissipated by generating a vortex in the vicinity of the water-permeable hole (slit) on the front wall is efficiently used for the rotation of the rotating body. That is, from the viewpoint of wave extinction, energy loss due to generation of excessive vortices can be prevented from the viewpoint of power generation while dissipating wave energy as rotational energy of the rotating body. Therefore, power generation efficiency can be improved by using wave energy that has been intentionally dissipated in the past as an energy source for power generation while maintaining quietness.
- a wave power generation system is the wave power generation system according to the first aspect, wherein adjacent rotating bodies included in the rotating body row are configured to rotate in opposite directions. ing.
- the movement of the adjacent rotating body does not interfere, and the water flow can pass through the rotating body row smoothly. Therefore, the power generation efficiency can be further improved.
- the wave power generation system is the wave power generation system according to the first aspect or the second aspect, and further includes at least one of a first rectification member and a second rectification member.
- a first rectification member Between the rotating shafts of adjacent rotating bodies included in the rotating body row, an inflow region where waves flowing from the offshore side to the impermeable wall side pass, or waves flowing out from the impermeable wall side to the offshore side pass. It becomes a spill area.
- At least one of the inflow region and the outflow region is formed.
- the first rectification member is disposed in the vicinity of the outflow region on the offshore side, and guides a wave flowing from the offshore side to the impermeable wall side to the inflow region.
- the second rectifying member is disposed in the vicinity of the impermeable wall side of the inflow region, and guides a wave flowing out from the impermeable wall side to the offshore side to the outflow region.
- the first rectifying member guides the wave that flows into the impermeable wall side to the inflow region, and / or the second rectifying member causes the wave that tries to flow out from the impermeable wall side. Guided to the area. That is, the wave that the first rectifying member is to flow into can be guided to the inflow region without stagnation, and / or the wave that the second rectification member is to flow out can be guided to the outflow region without stagnation. Therefore, the power generation efficiency can be further improved.
- the wave power generation system is the wave power generation system according to the third aspect, wherein the rotating body included in the row of rotating bodies includes a portion corresponding to the inflow region and the outflow region. They are arranged at different intervals from the corresponding locations.
- a wave power generation system is the wave power generation system according to any of the first to fourth aspects, wherein the rotating bodies included in the rotating body row are arranged at unequal intervals. Has been.
- a wave power generation system is the wave power generation system according to any one of the first to fifth aspects, wherein the wave power generation system extends in a horizontal direction from the impermeable wall and supports the rotating body. An upper wall is further provided.
- the impervious wall and the rotating body can be unitized, installation work at the site can be facilitated.
- the wave power generation system according to the seventh aspect of the present invention is the wave power generation system according to any one of the first to fifth aspects, and further includes a caisson.
- the caisson includes the impervious wall, and a bottom part and an upper wall part extending from the lower part and the upper part of the impervious wall to the offshore side, respectively.
- a wave power generation system is the wave power generation system according to any one of the first to seventh aspects, wherein the rotating body row is installed, and It further includes a foundation whose water depth is shallower than the water depth at the offshore side.
- the installation location of the rotating body is raised by the base, and the rotating body is installed at a position where the water level is lower (shallow) than the location on the offshore side. Therefore, in this case, the traveling speed of the wave passing between the rotating bodies is increased, and the dissipation of the wave energy is increased. Therefore, the wave reflectance can be reduced.
- the wave power generation system according to the ninth aspect of the present invention is the wave power generation system according to the eighth aspect, wherein the base has a vertical surface facing the offshore side.
- a step with a sudden change in water depth is formed near the offshore side of the water turbine, and the flow velocity of the incoming waves increases. Therefore, the wave reflectance is further reduced, and the power generation efficiency is further improved.
- a wave power generation system is the wave power generation system according to any one of the first to ninth aspects, wherein the rotating body rotates in a constant direction regardless of a wave direction. It is a water wheel.
- the rotating body rotates in the same direction both when the wave is applied to the impermeable wall and when the wave is drawn. Therefore, the power generation efficiency can be further improved.
- a wave power generation system is the wave power generation system according to the tenth aspect, wherein the rotating body is a Savonius turbine.
- a Savonius turbine is used as the rotating body. Therefore, it is possible to construct a power generation system that generates a large torque even at a low speed and is easy to operate even at a low flow rate.
- a wave power generation system is the wave power generation system according to any one of the first to eleventh aspects, wherein a rotation axis of the rotating body extends in a vertical direction.
- vertical direction includes the case of being completely parallel to the vertical direction and the case of being substantially parallel to the vertical direction, unless otherwise specified.
- the generator can be easily installed at an appropriate position on the water.
- energy loss can be prevented from the viewpoint of power generation while dissipating wave energy as rotational energy of the rotating body from the viewpoint of wave suppression. Therefore, power generation efficiency can be improved by using wave energy that has been intentionally dissipated in the past as an energy source for power generation while maintaining quietness.
- FIG. 1 is a longitudinal sectional view of a wave power generation system according to a first embodiment of the present invention.
- II-II sectional drawing of FIG. The longitudinal cross-sectional view of the wave power generation system which concerns on 2nd Embodiment of this invention.
- IV-IV sectional drawing of FIG. The transverse cross section of the wave power generation system concerning a 3rd embodiment of the present invention.
- the cross-sectional view of the wave power generation system which concerns on 4th Embodiment of this invention.
- the cross-sectional view of the wave power generation system which concerns on a modification.
- the longitudinal cross-sectional view of the wave power generation system which concerns on another modification.
- FIG. 1 is a side view of experimental equipment including a wave power generation system according to Embodiment 1.
- 1 is a side view of a power measurement system included in an experimental facility in Example 1.
- the graph which shows the comparison result of the reflectance in Example 1 (point) and a comparative example (curve) (in the case of Ds / h 0.350).
- the graph which shows the comparison result of the reflectance in Example 1 (point) and a comparative example (curve) (in the case of Ds / h 0.525).
- the graph which shows the relationship between the reflectance in Example 1, and load torque (in the case of Ds / h 0.215).
- the graph which shows the relationship between the reflectance in Example 1, and load torque (in the case of Ds / h 0.350).
- the graph which shows the relationship between the reflectance in Example 1, and load torque (in the case of Ds / h 0.525).
- FIG. 2 The top view (upper figure) and side view (lower figure) of the experimental installation containing the wave power generation system which concern on Example 2.
- FIG. The front view of the wave power generation system which concerns on Example 2.
- FIG. The top view of the wave power generation system which concerns on Example 2.
- the graph (case 2) which shows the relationship between the energy conversion efficiency in Example 2, and load torque.
- the graph which shows the relationship between the energy conversion efficiency and load torque in Example 2 (case 3).
- FIG. 1 is a longitudinal sectional view of the wave power generation system 1
- FIG. 2 is a sectional view taken along the line II-II in FIG.
- the wave power generation system 1 is a structure that is installed in the sea and has a function as a breakwater and a function as a power generation system.
- the wave power generation system 1 includes an impermeable wall 10 and a water turbine row 2 (rotating body row) installed on the offshore side of the impermeable wall 10.
- the impermeable wall 10 extends so as to intersect the traveling direction of the waves, and is installed so as to separate the shore side and the offshore side.
- the water turbine row 2 is configured by arranging a plurality of water turbines 20 (rotating bodies) along a direction in which the impermeable wall 10 extends in a plan view. As shown in FIG. 2, the line connecting the rotation shafts 21 of the plurality of water turbines 20 constituting the water turbine row 2 and the impermeable wall 10 are substantially parallel in a plan view.
- the impermeable wall 10 is a rectangular flat plate that is installed on a base 11 formed on the seabed and stands upright from the base 11. From the upper part of the impervious wall 10, a rectangular roof portion 12 (upper wall part) protrudes to the offshore side so as to be orthogonal to the impervious wall 10. And the rectangular bottom 13 protrudes so as to be orthogonal to the impermeable wall 10. That is, the roof portion 12 and the bottom portion 13 spread in the horizontal direction.
- the bottom portion 13 is installed on the base 11 and firmly supports the impermeable wall 10 and the roof portion 12 formed integrally with the bottom portion 13.
- the water turbine 20 has a rotating shaft 21 extending in the vertical direction, and a lower portion of the rotating shaft 21 is rotatably fixed to the bottom portion 13.
- the generator 3 is installed in the lower part of the roof part 12, and the upper part of the rotating shaft 21 is received by the generator 3 so that rotation is possible.
- the impermeable wall 10, the roof portion 12, and the bottom portion 13 constitute a caisson, and are made of concrete, for example.
- the foundation 11 can also be made of concrete.
- the foundation 11 also plays a role of stably supporting the caisson and the water wheel train 2, but can also reduce the wave reflectance. It is also possible to increase power generation efficiency. That is, the installation position of the water turbine 20 is raised by the base 11 (and the bottom 13), so that the water turbine 20 is installed at a low (shallow) water level. In this case, the wave passing between the water turbines 20 This is because the traveling speed of the wave increases and the dissipation of wave energy increases.
- the base 11 of the present embodiment extends between the impermeable wall 10 and the water turbine row 2 and is inclined downward from the vicinity of the water turbine row 2 near the offshore side toward the offshore side.
- the impervious wall 10 is a structure that forms a breakwater, reflects waves from the offshore side, and returns them to the offshore side.
- the impermeable wall 10 has a vertical surface on the offshore side.
- the water level of the sea surface varies depending on tides and weather conditions, but the impervious wall 10 according to the present embodiment has a height that exceeds the sea surface at an arbitrary time under general weather conditions. is there.
- the impervious wall 10 and the water wheel train 2 are arranged at a predetermined interval as if constituting a water reserving chamber.
- the wave that has reached the water turbine train 2 from the offshore side passes through the water turbine train 2 and collides with the impervious wall 10 to be reflected. Then, the reflected wave passes through the water wheel train 2 again and returns to the offshore side. During this time, the water turbine 20 rotates by the action of the waves passing through the water turbine train 2, and the energy of the waves is converted into rotational energy of the water turbine 20. That is, the water wheel train 2 plays a role of a wave extinguishing work that dissipates wave energy together with the impermeable wall 10. Further, as described above, the water turbine row 2 is installed on the offshore side of the impermeable wall 10, but a conventional permeable front wall (see Patent Document 1) having a water-permeable hole is not installed. In this sense, it can be said that the water turbine train 2 is an alternative to the permeable front wall used in conventional breakwaters.
- the water wheel 20 according to the present embodiment is a water wheel that rotates in a certain direction regardless of the wave direction. Therefore, each water wheel 20 rotates in the same direction at the time of a spilling wave and a drawing wave with respect to the impermeable wall 10 and contributes to power generation.
- each turbine 20 according to the present embodiment includes a plurality of (in this embodiment, three stages) Savonius turbines 20A to 20C that are stacked in the vertical direction and have a common rotating shaft 21. Have. Therefore, the water turbine 20 has a general property of the Savonius turbine, such that it generates a large torque at a low rotation and is easy to operate at a low flow rate.
- each turbine 20 can be configured in a single stage.
- the water turbine 20 is arranged so that at least a part of the Savonius turbines 20A to 20C arranged in the vertical direction exist below the sea surface at an arbitrary time under general weather conditions. Therefore, the wave power generation system 1 can always rotate all the water turbines 20 without being affected by the tidal wave.
- the Savonius turbines 20A to 20C each include two semicircular turbine blades 22 in a cross-sectional view. These two water turbine blades 22 are arranged in such a positional relationship that when one of them is rotated by 180 ° around the rotation shaft 21, it overlaps the other. Further, the turbine blades 22 of the Savonius turbine adjacent in the vertical direction are arranged at a position shifted by a predetermined angle around the rotation shaft 21, and thereby the rotation of the entire turbine 20 is made smooth. In the present embodiment, the angle of this deviation is set to 120 ° obtained by dividing 360 ° by 3 which is the number of stages of the Savonius turbine, and the smoothness of rotation is optimized.
- two adjacent water turbines 20 included in the water turbine train 2 are configured to rotate in opposite directions. That is, in the water wheel train 2, the clockwise water wheels 20 and the counterclockwise water wheels 20 are alternately arranged. As a result, the movement of the water turbine 20 or the direction of the water flow accompanying this does not interfere between adjacent water turbines 20, and the waves can pass through the water turbine train 2 smoothly.
- the plurality of water turbines 20 included in the water turbine row 2 have the same structure except that the rotation directions of two adjacent water turbines are different.
- staggered rotation configuration The configuration in which two adjacent water turbines included in the water turbine row 2 rotate in opposite directions (hereinafter referred to as staggered rotation configuration) is not limited to the wave power generation system 1 according to the present embodiment, but various wave power generation systems. Can be employed.
- the staggered rotation configuration can be applied to a water turbine row arranged in a water break chamber of a breakwater having a permeable front wall on the offshore side of an impermeable wall as described in Patent Document 1. .
- the generator 3 receives the rotational force via the rotating shaft 21 and generates power.
- the structure of the generator which converts the rotational energy of a water turbine into electric power is known, detailed description is abbreviate
- the configuration of the generator 3 is not limited as long as the rotational energy of the rotating shaft 21 can be converted into electric power. The same applies to the arrangement of the generator 3, and the generator 3 can be installed not only above the rotating shaft 21 but at an arbitrary position.
- the electric power generated by the generator 3 is transmitted to a land-side substation or the like via a power transmission facility (not shown). Since the wave power generation system 1 is normally installed near the sea in order to fulfill the function of a breakwater, power loss due to power transmission is suppressed.
- the wave energy is efficiently converted into the rotational energy of the water turbine 20, and the rotational energy is converted into electric power by the generator 3.
- the wave energy is dissipated, the wave is dissipated, and power can be generated efficiently from the wave energy.
- a permeable front wall is omitted on the offshore side of the impermeable wall 10 on the breakwater, and a water turbine row 2 is installed instead.
- the energy of the wave is not dissipated by the vortex generated in the vicinity of the water-permeable hole in the front wall as in the conventional wave power generation system having the permeable front wall, and is efficient in the rotation of the water turbine row 2.
- the wave power generation system 1 can be realized as a port facility such as a fishing port, a commercial port, or an evacuation port.
- the wave power generation system 1 can be introduced relatively smoothly if the existing breakwater needs to be replaced due to deterioration or the like.
- FIG. 3 is a longitudinal sectional view of the wave power generation system 101
- FIG. 4 is a sectional view taken along the line IV-IV in FIG.
- the wave power generation system 101 is a structure that is installed in the sea and has a function as a breakwater and a function as a power generation system, and is common in many respects to the wave power generation system 1 according to the first embodiment.
- differences from the first embodiment will be mainly described, and the same components as those in the first embodiment will be denoted by the same reference numerals and detailed description thereof will be omitted.
- the wave power generation system 101 includes an impermeable wall 10, a roof portion 12 (upper wall portion), a bottom portion 13, a base 11, a water wheel train 2, and a generator 3, and a first rectifying member. 150 and the second rectifying member 160.
- the main difference between the wave power generation system 101 according to the present embodiment and the wave power generation system 1 according to the first embodiment is whether or not the first rectifying member 50 and the second rectifying member 60 are present. .
- the impermeable wall 10 extends in plan view while leaving a plurality of water turbines 120 (rotating bodies) at a certain distance from the impermeable wall 10 as in the first embodiment. It is configured by arranging along the direction.
- each turbine 120 is not a multi-stage configuration in which Savonius turbines are stacked in the vertical direction, but is a single-stage configuration.
- the Savonius turbine 120 according to the second embodiment may be configured in a multistage configuration.
- the water wheel 120 has a shaft upper part 131, a wing part 132, and a shaft lower part 133 in order from the top in the vertical direction.
- the wing portion 132 includes an upper flange 134, a lower flange 135, and a pair of water turbine blades 136.
- Each turbine blade 136 has a semi-cylindrical shape, and the turbine 120 is a Savonius type in which two turbine blades 136 are arranged 180 degrees rotationally symmetrical with respect to the rotating shaft 121 of the turbine 120. For this reason, like the first embodiment, the water wheel 120 can also rotate in only one direction.
- Each turbine blade 136 has an upper flange 134 connected to the upper end and a lower flange 135 connected to the lower end, and reaches the outer periphery of both flanges 134 and 135, but does not protrude outward from the outer periphery. Further, the upper part of the water turbine blade 136 is always exposed above the water surface 114 under general weather conditions.
- the shaft upper portion 131 and the shaft lower portion 133 are parallel to the impermeable wall 10 and are arranged at a certain distance from the impermeable wall 10.
- the lower end portion of the shaft upper portion 131 is connected to the center of the upper surface of the upper flange 134, and the shaft upper portion 131 and the upper flange 134 are coaxial.
- the shaft upper portion 131 extends in the vertical direction, and an upper end portion thereof is inserted into a through hole 115 provided in the roof portion 12, and is rotatably supported.
- the upper end portion of the shaft lower portion 133 is connected to the center of the lower surface of the lower flange 135, and the shaft lower portion 133 and the lower flange 135 are coaxial.
- the lower shaft portion 133 extends in the vertical direction, and a lower end portion thereof is inserted into a bearing hole 116 provided on the upper surface of the bottom portion 13 and is rotatably supported.
- the two adjacent water turbines 120 are also configured to rotate in opposite directions. That is, there are a water wheel 120 that rotates counterclockwise in plan view (hereinafter also referred to as the first water wheel 120A) and a water wheel that rotates clockwise in plan view (hereinafter also referred to as the second water wheel 120B).
- the water turbines 120 are alternately arranged along the arrangement direction.
- the adjacent first and second water turbines 120A and 120B have a line-symmetric shape with respect to a straight line that is equidistant from the rotating shaft 121 of both the water turbines 120A and 120B.
- the two water turbine blades 136 of the first water wheel 120A are both pushed by the wave so that the first water wheel 120A rotates counterclockwise in plan view.
- the two water turbine blades 136 of the second water turbine 120B are both pushed by the waves so that the second water turbine 120B rotates clockwise in plan view.
- the water turbines 120A and 120B adjacent to each other have the rotation directions opposite to each other. For this reason, between the rotating shaft 121 of the adjacent first water wheel 120A and the rotating shaft 121 of the second water wheel 120B, an inflow region 118 through which the wave F1 that flows from the offshore side to the impermeable wall 10 side passes, Or it becomes the outflow area
- the inflow areas 118 and the outflow areas 119 are alternately formed along the arrangement direction of the water turbines 120.
- a plurality of first rectifying members 150 are present to form a row, and a plurality of second rectifying members 160 are also present to form a row.
- the first rectifying member 150 and the second rectifying member 160 each extend in the vertical direction, each upper end portion is fixed to the lower surface of the roof portion 12, and each lower end portion is fixed to the upper surface of the bottom portion 13.
- the first rectifying member 150 and the second rectifying member 160 have a rectangular parallelepiped shape, and as shown in FIG. 4, the cross section (horizontal cross section) has a square shape.
- the dimensions of the diagonal lines of the square cross section of the first rectifying member 150 and the second rectifying member 160 are substantially the same as the diameters of the upper flange 134 and the lower flange 135 of the water turbine 120.
- the first rectifying member 150 is disposed in the vicinity of the outflow region 119 on the offshore side, and one of the four vertices of the cross section (hereinafter referred to as the first vertex 151) is directed to the outflow region 119 side. More specifically, in the first rectifying member 150, an imaginary line 142 passing through the first vertex 151 of the first rectifying member 150 and the diagonally second vertex 152 in the cross-sectional view is adjacent to the first water wheel 120 ⁇ / b> A and the first It arrange
- the virtual line 142 and the virtual line segment 141 are orthogonal.
- the first vertex 151 is located on the offshore side of the imaginary line segment 141, but the first rectifying member 150 enters a gap formed between the adjacent first and second water turbines 120A and 120B.
- the second rectifying member 160 is disposed in the vicinity of the impermeable wall 10 side of the inflow region 118, and one of the four vertices (hereinafter referred to as the first vertex 161) of the cross section thereof is directed toward the inflow region 118. ing. More specifically, the second straightening member 160 has a virtual line 144 passing through the first vertex 161 of the second straightening member 160 and the diagonally second vertex 162 in the cross-sectional view. It arrange
- the wave F ⁇ b> 1 about to flow into the impermeable wall 10 side is an angle corresponding to the second vertex 152 located on the offshore side of the first rectifying member 150 disposed on the downstream side of the outflow region 119. It is divided into left and right (up and down direction in FIG. Thereafter, the wave F1 pushes the inner peripheral surfaces of the water turbine blades 136 of the first water wheel 120A and the second water wheel 120B to rotate both water wheels 120A and 120B. At this time, the first water wheel 120A rotates counterclockwise and the second water wheel 120B rotates clockwise in plan view.
- the wave F1 is at the corner corresponding to the first vertex 161 located on the offshore side of the second rectifying member 160 disposed on the downstream side of the inflow region 118. It collides and flows into the outflow area 119 without stagnation.
- the wave F ⁇ b> 2 about to flow out from the impermeable wall 10 side is at a corner corresponding to the second vertex 162 located on the impermeable wall 10 side of the second rectifying member 160 disposed on the downstream side of the inflow region 118.
- the collision is divided into left and right and led to the outflow area 119.
- the wave F2 pushes the inner peripheral surfaces of the water turbine blades 136 of the first water wheel 120A and the second water wheel 120B to rotate both water wheels 120A and 120B.
- the first water wheel 120A rotates counterclockwise and the second water wheel 120B rotates clockwise in plan view.
- the wave F2 corresponds to the first vertex 151 located on the impermeable wall 10 side of the first rectifying member 150 disposed on the downstream side of the outflow region 119 after rotating the first water wheel 120A and the second water wheel 120B. It collides with the corner and flows out offshore without itchiness.
- the entire waves F1 and F2 that are about to flow in and out are guided to the inflow region 118 and the outflow region 119 by the first rectifying member 150 and the second rectifying member 160, and the first water turbine 120A and the second water wheel 120B are made to flow.
- This breakwater can convert most of the wave energy into the rotational energy of the water wheel 120 and can be wave-dissipated.
- the waves F1 and F2 guide the water flow to the inner peripheral surface of the water turbine blade 136 of the water turbine 120 by the first rectifying member 150 and the second rectifying member 160, but do not guide the water flow to the outer peripheral surface of the water turbine blade 136.
- the rotation resistance of the water wheel 120 does not become resistance.
- the generator 3 receives the rotational force via the shaft upper portion 131 and generates power.
- the generator 3 is arrange
- the arrangement and configuration of the generator 3 can be appropriately selected.
- the electric power generated by the generator 3 is transmitted to a land-side substation or the like via a power transmission facility (not shown).
- the impervious wall 10 can also be installed so that the coast 125 may be touched or substantially contacted.
- FIG. 5 is a cross-sectional view of the wave power generation system 201.
- the wave power generation system 201 is common in many respects to the wave power generation systems 1 and 101 according to the first and second embodiments. In the following description, differences from the first and second embodiments will be mainly described. The same reference numerals are given to the same components as those in the first and second embodiments, and detailed description thereof will be omitted.
- the wave power generation system 201 includes an impermeable wall 10, a roof portion 12 (upper wall portion), a bottom portion 13, a base 11, a water wheel train 2, and a generator 3.
- the first straightening member 250 and the second straightening member 260 are provided.
- the main difference between the wave power generation system 201 according to the present embodiment and the wave power generation system 101 according to the second embodiment is the distance between the water turbines 120 included in the water turbine train 2.
- the adjacent first water wheel 120A and the second water wheel 120B are arranged substantially without a gap. By doing so, it is possible to reduce the amount of waves that pass through the gap between the first water wheel 120A and the second water wheel 120B without substantially contributing to the rotation of the water wheels 120A and 120B. That is, power generation efficiency can be improved.
- a plurality of first rectifying members 250 exist to form a row
- a plurality of second rectifying members 260 also exist to form a row.
- the first and second rectifying members 250 and 260 are different from the first and second rectifying members 150 and 160 according to the second embodiment only in the cross-sectional shape, and have the same configuration in other points. .
- the cross-sectional shape of the first rectifying member 250 is a shape having four vertices surrounded by a pair of adjacent curves 253 and a pair of adjacent line segments 254.
- the first rectifying member 250 is disposed in the vicinity of the outflow region 119 on the offshore side, and is one of the four vertices of the cross section, and an intersection of a pair of curves 253 (hereinafter referred to as a first vertex 251). It faces the outflow area 119 side.
- the second vertex 252 is an intersection of a pair of line segments 254.
- a virtual line 242 passing through the first vertex 251 of the first rectifying member 250 and the diagonally second vertex 252 in the cross-sectional view is adjacent to the first turbine 120 ⁇ / b> A and the first It arrange
- the virtual line 242 and the virtual line segment 241 are orthogonal to each other.
- the first vertex 251 is located on the offshore side of the virtual line segment 241, but the first rectifying member 250 enters a gap formed between the adjacent water turbines 120.
- a curved line 253 extending from the corner corresponding to the first vertex 251 in the left-right direction (the vertical direction in FIG. 5, the same applies hereinafter) includes the upper flange 134 and the lower flange 135 of the water turbine 120. It is concentric and has a slightly larger arc shape.
- the cross-sectional shape of the second rectifying member 260 is a shape having four vertices surrounded by a pair of adjacent curves 263 and a pair of adjacent line segments 264.
- the second rectifying member 260 is disposed in the vicinity of the impermeable wall 10 side of the inflow region 118, and is one of the four vertices of the cross section thereof, and is an intersection of a pair of curves 263 (hereinafter referred to as the first vertex 261). Is directed to the inflow region 118 side.
- the second vertex 262 is an intersection of a pair of line segments 264.
- the second straightening member 260 has a virtual line 244 passing through the first vertex 261 of the second straightening member 260 and the diagonally second vertex 262 in the cross-sectional view, and the adjacent first turbine 120A and the second It arrange
- the virtual line 244 and the virtual line segment 243 are orthogonal to each other.
- the first vertex 261 is located on the side of the impermeable wall 10 with respect to the imaginary line segment 243, the second rectifying member 260 enters a gap formed between the adjacent water turbines 120.
- a curved line 263 extending from the corner corresponding to the first vertex 261 in the left-right direction includes the upper flange 134 and the lower flange 135 of the turbine 120. It is concentric and has a slightly larger arc shape.
- the wave power generation system 201 can improve the power generation efficiency compared with the wave power generation systems 1 and 101 already described.
- FIG. 6 is a cross-sectional view of the wave power generation system 301.
- the wave power generation system 301 is common in many respects to the wave power generation systems 1, 101, 201 according to the first to third embodiments. In the following description, differences from the first to third embodiments will be mainly described. The same components as those in the first to third embodiments will be denoted by the same reference numerals, and detailed description thereof will be omitted.
- the wave power generation system 301 includes an impermeable wall 10, a roof portion 12 (upper wall portion), a bottom portion 13, a base 11, a water wheel train 2, and a generator 3.
- the first straightening member 350 and the second straightening member 360 are provided.
- the main difference between the wave power generation system 301 according to the present embodiment and the wave power generation systems 101 and 202 according to the second and third embodiments is in the distance between the water turbines 120 included in the water turbine train 2.
- the water turbines 120 included in the water turbine row 2 are arranged at unequal intervals.
- the water turbines 120 included in the water turbine row 2 are arranged at different positions at locations corresponding to the inflow region 118 and locations corresponding to the outflow region 119.
- the interval between adjacent water turbines 120 at a position corresponding to the outflow region 119 is wider than the interval between adjacent water turbines 120 at a position corresponding to the inflow region 118, but may be reversed as shown in FIG. Is possible.
- the degree of freedom of the installation position of the water turbine 120 is high. Therefore, the amount of wave inflow and outflow to the breakwater that improves the power generation efficiency is determined for each installation location, and at the same time, each interval between adjacent water turbines 120 included in the water turbine row 2 is set separately. be able to. In particular, it is significant that the interval at the position corresponding to the inflow region 118 and the interval at the position corresponding to the outflow region 119 can be set separately.
- a Savonius turbine is used as the rotating body, but the present invention is not limited to this, and other types of turbines can also be used.
- a water turbine that rotates in a certain direction regardless of the direction of the waves so that power generation can be easily performed at the time of spilling and at the time of wave drawing.
- a cross flow water wheel in addition to the Savonius water wheel.
- a water wheel deformed so as to have a different number of water wheel blades such as three or four can be used.
- the rotation shaft is arranged separately above and below the central wing, but may pass through the wing 132.
- the upper part of the wing part 132 is exposed above the water surface, but may be always submerged.
- the wave power generation system is installed in the sea, but it can also be installed in a river or a lake.
- one of the first rectifying member and the second rectifying member may be omitted.
- the offshore side of the base 11 was comprised so that a slope might be formed with respect to a perpendicular direction.
- a base 11A having a vertical surface 111A on the offshore side may be provided instead of the base 11, instead of the base 11, a base 11A having a vertical surface 111A on the offshore side may be provided.
- a base 11 ⁇ / b> B may be further formed on the bottom portion 13 provided on the base 11.
- the base 11B in FIG. 9 is formed substantially only below the water wheel 20 and is a rectangular parallelepiped base that does not reach the impervious wall 10 in a longitudinal sectional view, but reaches the impervious wall 10 through the base 11B. It can also be a foundation.
- the base is not a trapezoidal shape as shown in FIG.
- the water depth changes abruptly near the offshore side and immediately below the water turbine 20.
- a step is formed, the wavelength of the incoming wave changes, and the flow velocity increases. Therefore, in this case, the effect of reducing the wave reflectance and the effect of improving the power generation efficiency are expected.
- Example 1 of the present invention will be described. However, the present invention is not limited to the following Example 1.
- the power measurement system shown in FIG. 12 was installed instead of the generator.
- the rotating shaft of the water turbine (water turbine shaft) was supported at its lower end by using a ball bearing bearing so that friction was minimized.
- the upper end of the water wheel axis is connected to the magnetic brake, the water axle gave load torque T q [N ⁇ m] by the magnetic brake.
- the magnetic brake Perma-Tork HC01-1 manufactured by Nippon Sohatsu Co., Ltd. was used.
- an accelerometer was fixed to the turbine shaft, and the rotation speed (angular velocity) R E [rps] of the turbine was measured for 30 to 80 seconds after the start of wave formation at a sampling frequency of 100 Hz.
- the sampling frequency of the wave height meter was 100 Hz.
- the diameter of the water wheel should be determined according to the water depth and the wave period. Further, when the diameter of the water wheel is set to about 20% to 50% of the water depth, it is possible to realize a reflectance of about 30% to 80%. In particular, the diameter of the water wheel is set to about 50% of the water depth. In some cases, a reflectivity of about 30% to 50% can be achieved.
- P p below is the acquired power per unit width obtained by the rotation of the water turbine, and P w is the wave energy per unit width.
- ⁇ is the density of water and g is the acceleration of gravity.
- R E in the following formula is an average rotation speed.
- the power generation efficiency (acquired power efficiency) for wave energy generated by Savonius turbines is about 5%.
- the maximum value of the acquired power efficiency K e becomes 10% or more, high power It turns out that efficiency is expected.
- Example 2 of the present invention will be described.
- the present invention is not limited to the following Example 2.
- an impermeable wall was installed on the l [m] shore side further from the rotation axis of the water wheel train.
- the diameter D s [m] of the Savonius turbine was set to 0.072.
- the number of water turbines included in the water turbine train is six, and the water turbine train has a staggered rotation configuration in which adjacent water turbines rotate in reverse.
- a water wheel distance D [m] 1.1D s.
- Each turbine included in the turbine row is configured by changing the three-stage Savonius turbine described in the first embodiment to a two-stage configuration.
- a rectangular parallelepiped step 11A that spreads l '[m] from the impervious wall to the offshore side and widened by the width of the wave-making water tank in the width direction was prepared, and a water turbine row was arranged on the step 11A.
- Example 2 In the wave power generation system according to Example 2, a power measurement system similar to that shown in FIG. 12 was installed instead of the generator, and a load torque T q [N ⁇ m] was applied to the water wheel shaft.
- an electromagnetic current meter made by Alec Electronics Co., Ltd. was installed at a position between the turbines (offshore) and 0.08 m below the static water surface, and the flow velocity between the turbines was measured. Further, the rotational speed ⁇ of the water turbine was measured at a sampling frequency of 100 Hz using an accelerometer (sensor controller) manufactured by ATR Promotions Inc. attached to the upper end of the water wheel shaft.
- case 2 with only the water wheel train has a lower reflectance than the case 1 under any l ′ conditions. Furthermore, in the case3 provided waterwheel column on step 11A, although almost the same K r and case2 in short-period zone, decline significant K r is observed in long period range, the step 11A It turned out that this tendency is so remarkable that it is long. On the other hand, Vmax / umax of case 3 is larger than that of case 2. Therefore, by installing a water wheel on step 11A, the energy dissipation becomes faster flow rate through the inter-turbine is increased, the reflectance K r is considered to have reduced.
- the reflectivity Kr tends to be the lowest in case 3, the next lowest in case 2, and the maximum in case 1. Accordingly, it has been confirmed that the wave-dissipating performance is improved by the water wheel train, and further, when the water wheel train is installed on the step 11A, the wave-dissipating performance is further improved.
- the maximum flow velocity Vmax passing through is shown. From the figure, the larger the l / l ', i.e., that there is a tendency that the minimum value of about K r installation position of the water wheel column is offshore step 11A decreases were confirmed. Therefore, it was found that the water turbine train is preferably arranged in the vicinity of the offshore end of Step 11A from the viewpoint of wave extinction.
- Wave power generation system Water wheel train (rotating body train) 3 Generator 10 Impervious Wall 11, 11A, 11B Base (Step) 12 Roof part (upper wall part) 20,120 Water wheel (rotary body) 120A 1st water wheel 120B 2nd water wheel 21, 121 Rotating shaft 118 Inflow area 119 Outflow area 150, 250, 350 First rectifying member 160, 260, 360 Second rectifying member
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Abstract
Description
本発明は、波のエネルギーを消散させるとともに、波のエネルギーから発電を行う波力発電システムに関する。 The present invention relates to a wave power generation system that dissipates wave energy and generates power from the wave energy.
近年、化石燃料の枯渇や地球温暖化等の環境問題への対策として、再生可能エネルギー(自然エネルギー)を利用した発電が注目を集めている。これらのうち波力発電は、地球表面の7割もの領域を覆う海において発生する波力を利用するものであり、有力なエネルギー源として着目されている。 In recent years, power generation using renewable energy (natural energy) has attracted attention as a countermeasure against environmental problems such as depletion of fossil fuels and global warming. Of these, wave power generation uses wave power generated in the sea covering 70% of the earth's surface, and has attracted attention as a powerful energy source.
しかしながら、船舶の航行安全や漁場確保等の観点から、海洋に構造物を設置することが厳しく制限される場合があり、波力発電システムの設置が困難となる場合がある。かかる問題に鑑み、特許文献1は、港湾海域に比較的多く設置されている防波堤の遊水室内に水車を設置した波力発電システムを開示している。すなわち、特許文献1の波力発電システムは、既存の港湾インフラを利用するため設置が容易となり、更には、発電装置や送電施設の付加に掛かるコストを低減することもできる。
However, from the viewpoints of ship navigation safety and securing of fishing grounds, the installation of structures in the ocean may be severely restricted, and the installation of a wave power generation system may be difficult. In view of such a problem,
ところで、特許文献1では、岸側に不透過壁と、沖側に縦スリットを有する透過性の前壁とを備えた防波堤が利用される。この種の防波堤は、不透過壁で波を反射させることで岸側の静穏性を確保するととともに、前壁の縦スリットの近傍で発生する渦により、波のエネルギーを消散させる。これにより、不透過壁における波の反射率を低下させ、岸側だけでなく、船舶等の通過する沖側の静穏性をも確保することができる。
By the way, in
しかしながら、透過性の前壁によって波のエネルギーを消散させることは、消波の観点からは必要に思われるが、発電の観点からは非効率である。 However, it seems necessary to dissipate wave energy by the permeable front wall from the viewpoint of wave dissipation, but it is inefficient from the viewpoint of power generation.
本発明は、静穏性を保ちつつ、発電効率を向上させることができる波力発電システムを提供することを目的とする。 The present invention aims to provide a wave power generation system capable of improving power generation efficiency while maintaining quietness.
本発明の第1観点に係る波力発電システムは、防波堤と共に用いられ、波のエネルギーを消散させるとともに、前記波のエネルギーから発電を行う波力発電システムであって、回転体列と、発電機とを備える。前記防波堤は、水中に設置され、不透過壁を有するが、前記不透過壁の沖側に透過性の前壁を有さない防波堤である。前記回転体列は、前記不透過壁の沖側において、平面視において前記不透過壁の延びる方向に沿って配列された複数の回転体からなる。前記発電機は、前記複数の回転体の回転エネルギーを電力に変換する。 A wave power generation system according to a first aspect of the present invention is a wave power generation system that is used together with a breakwater to dissipate wave energy and generate electric power from the wave energy. With. The breakwater is a breakwater that is installed in water and has an impermeable wall, but does not have a permeable front wall on the offshore side of the impermeable wall. The rotating body row includes a plurality of rotating bodies arranged on the offshore side of the impermeable wall along a direction in which the impermeable wall extends in a plan view. The generator converts rotational energy of the plurality of rotating bodies into electric power.
ここでは、防波堤における不透過壁の沖側において、透過性の前壁が設置されることなく、これに代えて、回転体列が設置される。これにより、従来、前壁の透水孔(スリット)の近傍において渦を発生させることにより消散させられていた波のエネルギーは、回転体の回転に効率的に用いられることになる。すなわち、消波の観点からは、回転体の回転エネルギーとして波のエネルギーを消散させつつも、発電の観点からは、過剰な渦の発生によるエネルギーロスを防ぐことができる。従って、静穏性を保ちつつ、従来、意図的に消散させられていた波のエネルギーを発電のエネルギー源として利用することにより、発電効率を向上させることができる。 Here, on the shore side of the impermeable wall on the breakwater, a transmissive front wall is not installed, but a rotating body row is installed instead. Thereby, conventionally, the energy of the wave that has been dissipated by generating a vortex in the vicinity of the water-permeable hole (slit) on the front wall is efficiently used for the rotation of the rotating body. That is, from the viewpoint of wave extinction, energy loss due to generation of excessive vortices can be prevented from the viewpoint of power generation while dissipating wave energy as rotational energy of the rotating body. Therefore, power generation efficiency can be improved by using wave energy that has been intentionally dissipated in the past as an energy source for power generation while maintaining quietness.
本発明の第2観点に係る波力発電システムは、第1観点に係る波力発電システムであって、前記回転体列に含まれる隣り合う回転体は、相反する方向に回転するように構成されている。 A wave power generation system according to a second aspect of the present invention is the wave power generation system according to the first aspect, wherein adjacent rotating bodies included in the rotating body row are configured to rotate in opposite directions. ing.
ここでは、隣接する回転体の動きが干渉することがなく、水流がスムーズに回転体列を通過することができる。従って、発電効率をさらに向上させることができる。 Here, the movement of the adjacent rotating body does not interfere, and the water flow can pass through the rotating body row smoothly. Therefore, the power generation efficiency can be further improved.
本発明の第3観点に係る波力発電システムは、第1観点又は第2観点に係る波力発電システムであって、第1整流部材及び第2整流部材の少なくとも一方をさらに備える。前記回転体列に含まれる隣り合う回転体の回転軸間が、沖側から前記不透過壁側に流入する波が通過する流入領域、又は前記不透過壁側から沖側へ流出する波が通過する流出領域となる。前記流入領域及び前記流出領域は、各々少なくとも1つ形成される。前記第1整流部材は、前記流出領域の沖側の近傍に配置され、沖側から前記不透過壁側に流入する波を前記流入領域に導く。前記第2整流部材は、前記流入領域の前記不透過壁側の近傍に配置され、前記不透過壁側から沖側へ流出する波を前記流出領域に導く。 The wave power generation system according to the third aspect of the present invention is the wave power generation system according to the first aspect or the second aspect, and further includes at least one of a first rectification member and a second rectification member. Between the rotating shafts of adjacent rotating bodies included in the rotating body row, an inflow region where waves flowing from the offshore side to the impermeable wall side pass, or waves flowing out from the impermeable wall side to the offshore side pass. It becomes a spill area. At least one of the inflow region and the outflow region is formed. The first rectification member is disposed in the vicinity of the outflow region on the offshore side, and guides a wave flowing from the offshore side to the impermeable wall side to the inflow region. The second rectifying member is disposed in the vicinity of the impermeable wall side of the inflow region, and guides a wave flowing out from the impermeable wall side to the offshore side to the outflow region.
ここでは、隣り合う回転体の回転軸間が波の流入領域又は流出領域となる。なお、回転体列に含まれる隣り合う回転体が相反する方向に回転する場合には、流入領域及び流出領域は交互に形成される。また、ここでは、第1整流部材により、不透過壁側に流入しようとする波が流入領域に導かれ、及び/又は、第2整流部材により、不透過壁側から流出しようとする波が流出領域に導かれる。すなわち、第1整流部材が流入しようとする波を淀みなく流入領域へ導き、及び/又は第2整流部材が流出しようとする波を淀みなく流出領域へ導くことができる。従って、発電効率をさらに向上させることができる。 Here, between the rotating shafts of adjacent rotating bodies is a wave inflow region or an outflow region. In addition, when adjacent rotating bodies included in the rotating body row rotate in opposite directions, the inflow regions and the outflow regions are alternately formed. In addition, here, the first rectifying member guides the wave that flows into the impermeable wall side to the inflow region, and / or the second rectifying member causes the wave that tries to flow out from the impermeable wall side. Guided to the area. That is, the wave that the first rectifying member is to flow into can be guided to the inflow region without stagnation, and / or the wave that the second rectification member is to flow out can be guided to the outflow region without stagnation. Therefore, the power generation efficiency can be further improved.
本発明の第4観点に係る波力発電システムは、第3観点に係る波力発電システムであって、前記回転体列に含まれる回転体は、前記流入領域に対応する箇所と前記流出領域に対応する箇所とで異なる間隔を空けて配列されている。 The wave power generation system according to a fourth aspect of the present invention is the wave power generation system according to the third aspect, wherein the rotating body included in the row of rotating bodies includes a portion corresponding to the inflow region and the outflow region. They are arranged at different intervals from the corresponding locations.
本発明の第5観点に係る波力発電システムは、第1観点から第4観点のいずれかに係る波力発電システムであって、前記回転体列に含まれる回転体は、不等間隔で配列されている。 A wave power generation system according to a fifth aspect of the present invention is the wave power generation system according to any of the first to fourth aspects, wherein the rotating bodies included in the rotating body row are arranged at unequal intervals. Has been.
本発明の第6観点に係る波力発電システムは、第1観点から第5観点のいずれかに係る波力発電システムであって、前記不透過壁から水平方向に広がり、前記回転体を支持する上壁部をさらに備える。 A wave power generation system according to a sixth aspect of the present invention is the wave power generation system according to any one of the first to fifth aspects, wherein the wave power generation system extends in a horizontal direction from the impermeable wall and supports the rotating body. An upper wall is further provided.
ここでは、不透過壁と回転体等とをユニット化することができるため、現地での設置作業を容易にすることができる。 Here, since the impervious wall and the rotating body can be unitized, installation work at the site can be facilitated.
本発明の第7観点に係る波力発電システムは、第1観点から第5観点のいずれかに係る波力発電システムであって、ケーソンをさらに備える。前記ケーソンは、前記不透過壁と、前記不透過壁の下部及び上部からそれぞれ沖側に延びる底部及び上壁部とを有する。 The wave power generation system according to the seventh aspect of the present invention is the wave power generation system according to any one of the first to fifth aspects, and further includes a caisson. The caisson includes the impervious wall, and a bottom part and an upper wall part extending from the lower part and the upper part of the impervious wall to the offshore side, respectively.
本発明の第8観点に係る波力発電システムは、第1観点から第7観点のいずれかに係る波力発電システムであって、前記回転体列が設置され、前記回転体列の設置箇所の水深が沖側の箇所の水深よりも浅くなるようにされた土台をさらに備える。 A wave power generation system according to an eighth aspect of the present invention is the wave power generation system according to any one of the first to seventh aspects, wherein the rotating body row is installed, and It further includes a foundation whose water depth is shallower than the water depth at the offshore side.
ここでは、回転体の設置箇所が土台により嵩上げされ、当該設置箇所よりもさらに沖側の箇所と比べて水位の低い(浅い)位置に回転体が設置される。従って、この場合、回転体間を通過する波の進行速度が速くなり、波のエネルギーの散逸が大きくなる。よって、波の反射率を低下させることができる。 Here, the installation location of the rotating body is raised by the base, and the rotating body is installed at a position where the water level is lower (shallow) than the location on the offshore side. Therefore, in this case, the traveling speed of the wave passing between the rotating bodies is increased, and the dissipation of the wave energy is increased. Therefore, the wave reflectance can be reduced.
本発明の第9観点に係る波力発電システムは、第8観点に係る波力発電システムであって、前記土台は、沖側に面する垂直面を有する。 The wave power generation system according to the ninth aspect of the present invention is the wave power generation system according to the eighth aspect, wherein the base has a vertical surface facing the offshore side.
ここでは、水車の沖側の近傍で急激に水深が変化する段差が形成され、流入してくる波の流速が速くなる。従って、波の反射率がさらに低下し、発電効率がさらに向上する。 Here, a step with a sudden change in water depth is formed near the offshore side of the water turbine, and the flow velocity of the incoming waves increases. Therefore, the wave reflectance is further reduced, and the power generation efficiency is further improved.
本発明の第10観点に係る波力発電システムは、第1観点から第9観点のいずれかに係る波力発電システムであって、前記回転体は、波の方向によらず一定の方向に回転する水車である。 A wave power generation system according to a tenth aspect of the present invention is the wave power generation system according to any one of the first to ninth aspects, wherein the rotating body rotates in a constant direction regardless of a wave direction. It is a water wheel.
ここでは、不透過壁に対する寄せ波時においても、引き波時においても、回転体が同じ方向に回転する。従って、発電効率をさらに向上させることができる。 Here, the rotating body rotates in the same direction both when the wave is applied to the impermeable wall and when the wave is drawn. Therefore, the power generation efficiency can be further improved.
本発明の第11観点に係る波力発電システムは、第10観点に係る波力発電システムであって、前記回転体は、サボニウス水車である。 A wave power generation system according to an eleventh aspect of the present invention is the wave power generation system according to the tenth aspect, wherein the rotating body is a Savonius turbine.
ここでは、回転体として、サボニウス水車が利用される。従って、低回転でも大きなトルクが発生し、低流速でも稼働し易い発電システムを構築することができる。 Here, a Savonius turbine is used as the rotating body. Therefore, it is possible to construct a power generation system that generates a large torque even at a low speed and is easy to operate even at a low flow rate.
本発明の第12観点に係る波力発電システムは、第1観点から第11観点のいずれかに係る波力発電システムであって、前記回転体の回転軸は、鉛直方向に延びている。なお、本明細書において「鉛直方向」というときには、特に断らない限り、鉛直方向に完全に平行な場合と、鉛直方向に概ね平行な場合とが含まれるものとする。 A wave power generation system according to a twelfth aspect of the present invention is the wave power generation system according to any one of the first to eleventh aspects, wherein a rotation axis of the rotating body extends in a vertical direction. In the present specification, the term “vertical direction” includes the case of being completely parallel to the vertical direction and the case of being substantially parallel to the vertical direction, unless otherwise specified.
ここでは、発電機を水上等の適切な位置に容易に設置することができる。 Here, the generator can be easily installed at an appropriate position on the water.
本発明によれば、消波の観点からは、回転体の回転エネルギーとして波のエネルギーを消散させつつも、発電の観点からは、エネルギーロスを防ぐことができる。従って、静穏性を保ちつつ、従来、意図的に消散させられていた波のエネルギーを発電のエネルギー源として利用することにより、発電効率を向上させることができる。 According to the present invention, energy loss can be prevented from the viewpoint of power generation while dissipating wave energy as rotational energy of the rotating body from the viewpoint of wave suppression. Therefore, power generation efficiency can be improved by using wave energy that has been intentionally dissipated in the past as an energy source for power generation while maintaining quietness.
以下、図面を参照しつつ、本発明のいくつかの実施形態に係る波力発電システムについて説明する。 Hereinafter, a wave power generation system according to some embodiments of the present invention will be described with reference to the drawings.
<1.第1実施形態>
<1-1.波力発電システムの構成>
図1及び図2に、第1実施形態に係る波力発電システム1を示す。図1は、波力発電システム1の縦断面図であり、図2は、図1のII-II断面図である。波力発電システム1は、海中に設置され、防波堤としての機能と、発電システムとしての機能を有する構造物である。図1及び図2に示すとおり、波力発電システム1は、不透過壁10と、不透過壁10の沖側に設置される水車列2(回転体列)とを備える。不透過壁10は、波の進行方向と交差するように延び、岸側と沖側とを分離するように設置される。水車列2は、複数の水車20(回転体)を、平面視において不透過壁10の延びる方向に沿って配列することにより構成される。図2に示すように、水車列2を構成する複数の水車20の回転軸21を結んだ線と、不透過壁10とは、平面視において概ね平行である。
<1. First Embodiment>
<1-1. Configuration of wave power generation system>
1 and 2 show a wave
図1に示すとおり、不透過壁10は、海底に形成された土台11上に設置され、土台11上から鉛直方向に起立している矩形状の平板である。不透過壁10の上部からは、沖側へと矩形状の屋根部12(上壁部)が不透過壁10に直交するように突出しており、不透過壁10の下部からは、沖側へと矩形状の底部13が不透過壁10に直交するように突出している。すなわち、屋根部12及び底部13は、水平方向に広がっている。底部13は、土台11上に設置され、底部13と一体に形成されている不透過壁10及び屋根部12を強固に支持している。本実施形態に係る水車20は、鉛直方向に延びる回転軸21を有しており、回転軸21の下部が、底部13に回転可能に固定されている。屋根部12の下部には、発電機3が設置されており、回転軸21の上部は、発電機3に回転可能に受け取られている。不透過壁10と屋根部12と底部13とはケーソンを構成し、例えば、コンクリート製である。土台11も、コンクリート製とすることができる。
As shown in FIG. 1, the
土台11は、ケーソンや水車列2を安定的に支持する役割も果たすが、波の反射率を低下させることもできる。また、発電効率を上げることも可能である。すなわち、水車20の設置位置が土台11(及び底部13)により嵩上げされることで、水位の低い(浅い)位置に水車20が設置されることになり、この場合、水車20間を通過する波の進行速度が速くなり、波のエネルギーの散逸が大きくなるからである。本実施形態の土台11は、不透過壁10と水車列2との間を広がり、水車列2の沖側の近傍から沖側に向かって下方へ傾斜している。
The
不透過壁10は、防波堤を構成し、沖側からの波を反射させ、沖側へと返す役割を果たす構造物である。不透過壁10は、沖側に垂直面を有している。海面の水位は、潮の満ち引きや気象条件に応じて変動するが、本実施形態に係る不透過壁10は、一般的な気象条件下では、任意の時刻において海面を超える程度の高さである。また、不透過壁10と水車列2とは、遊水室を構成するかの如く、一定の間隔を空けて配置されている。
The
沖側から水車列2に達した波は、水車列2を通過して不透過壁10に衝突して反射する。そして、反射波は、水車列2を再度通過して、沖側へと戻ってゆく。この間、水車列2を通過する波の作用により、水車20が各々回転し、波のエネルギーが水車20の回転エネルギーへと変換される。すなわち、水車列2は、不透過壁10とともに、波のエネルギーを消散させる消波工の役割を果たす。また、不透過壁10の沖側には、上記のとおり水車列2が設置されているが、従来の透水孔を有する透過性の前壁(特許文献1参照)は設置されていない。この意味で、水車列2は、従来の防波堤に用いられている透過性の前壁の代替となるものと言える。
The wave that has reached the
本実施形態に係る水車20は、波の方向によらず一定の方向に回転する水車である。従って、不透過壁10に対する寄せ波時においても引き波時においても、各水車20は同じ方向に回転し、発電に寄与する。また、図1に示すように、本実施形態に係る各水車20は、共通の回転軸21を有する上下方向に積層された複数段(本実施形態では、三段)のサボニウス水車20A~20Cを有する。従って、水車20は、サボニウス水車の一般的な性質として、低回転で大きなトルクを発生し、低流速で稼働し易い性質を有する。なお、他の実施形態では、各水車20を一段構成とすることも可能である。本実施形態に係る水車20は、一般的な気象条件下では、上下方向に並ぶサボニウス水車20A~20Cの少なくとも一部が、任意の時刻において海面下に存在するように配置されている。従って、波力発電システム1は、波の干満の影響を受けることなく、常時、全ての水車20を回転させることができる。
The
図2に示すように、本実施形態に係るサボニウス水車20A~20Cは、各々、横断面視において半円状の水車翼22を2枚ずつ有する。これらの2枚の水車翼22は、一方を回転軸21の周りで180°回転させたときに他方に重なるような位置関係で配置されている。また、上下方向に隣接するサボニウス水車の水車翼22は、回転軸21の周りで所定の角度だけずれた位置に配置されており、これにより、水車20全体の回転が滑らかにされている。なお、本実施形態では、このずれの角度は、360°をサボニウス水車の段数である3で除した120°に設定されており、回転の滑らかさが最適化されている。
As shown in FIG. 2, the
また、図2に示すように、本実施形態に係る水車列2に含まれる隣り合う2つの水車20は、相反する方向に回転するように構成されている。すなわち、水車列2では、時計回りの水車20と、反時計回りの水車20とが交互に配列されている。その結果、隣接する水車20間で、水車20の動き、あるいはこれ伴う水流の向きが干渉することがなく、波がスムーズに水車列2を通過することができる。なお、水車列2に含まれる複数の水車20は、隣り合う2つの水車の回転方向が異なる点を除き、同様の構造を有している。
Further, as shown in FIG. 2, two
なお、水車列2に含まれる隣り合う2つの水車が相反する方向に回転する構成(以下、互い違い回転構成)は、本実施形態に係る波力発電システム1のみならず、様々な波力発電システムにおいて採用することができる。例えば、特許文献1に記載されるような、不透過壁の沖側に透過性の前壁を有する防波堤の遊水室内に配置される水車列に対しても、互い違い回転構成を適用することができる。
The configuration in which two adjacent water turbines included in the
以上のとおり、波の作用により水車20が回転すると、発電機3は、その回転力を回転軸21を介して受け取り、発電を行う。なお、水車の回転エネルギーを電力に変換する発電機の構成については、周知であるため、ここでは詳細な説明を省略する。発電機3は、回転軸21の回転エネルギーを電力に変換することができる限り、構成は問わない。発電機3の配置に関しても同様であり、回転軸21の上方に限らず、任意の位置に設置することができる。
As described above, when the
そして、発電機3で発電された電力は、図示されない送電設備を介して、陸側の変電所等に送電される。波力発電システム1は、防波堤の機能を果たすべく、通常近海に設置されているため、送電による電力損失が抑制されるようになっている。
And the electric power generated by the
以上より、波力発電システム1では、波のエネルギーは、水車20の回転エネルギーに効率的に変換され、当該回転エネルギーが発電機3により電力に変換される。これにより、波のエネルギーが消散し、消波が行われるとともに、波のエネルギーから効率的に発電することができる。
As described above, in the wave
<1-2.特徴> <1-2. Features>
波力発電システム1では、防波堤における不透過壁10の沖側において、透過性の前壁が省略されており、これに代えて、水車列2が設置されている。これにより、波のエネルギーは、透過性の前壁を備える従来の波力発電システムのように、前壁の透水孔の近傍において発生する渦により消散させられることなく、水車列2の回転に効率的に用いられる。すなわち、消波の観点からは、水車列2の回転エネルギーとして波のエネルギーを消散させつつも、発電の観点からは、渦の発生によるエネルギーロスが防止されている。従って、波力発電システム1では、静穏性が保たれるとともに、発電効率が高められている。
In the wave
波力発電システム1は、例えば、漁港や商業港、避難港等の港湾施設として実現することが可能である。また、波力発電システム1は、既存の防波堤が劣化等によって置換する必要が生じた場合等であれば、比較的円滑に導入を図ることができる。
The wave
<2.第2実施形態>
次に、第2実施形態に係る波力発電システム101について説明する。図3は、波力発電システム101の縦断面図であり、図4は、図3のIV-IV断面図である。波力発電システム101は、海中に設置され、防波堤としての機能と、発電システムとしての機能を有する構造物であり、第1実施形態に係る波力発電システム1と多くの点で共通する。以下では、第1実施形態との相違点を中心に説明することとし、第1実施形態と同様の構成には同様の参照符号を付して詳細な説明を省略する。
<2. Second Embodiment>
Next, the wave
波力発電システム101は、第1実施形態と同様に、不透過壁10、屋根部12(上壁部)、底部13、土台11、水車列2及び発電機3を備える他、第1整流部材150及び第2整流部材160を備える。本実施形態に係る波力発電システム101と、第1実施形態に係る波力発電システム1との主な相違点は、第1整流部材50及び第2整流部材60が存在するか否かにある。
Similar to the first embodiment, the wave
また、第2実施形態に係る水車列2は、第1実施形態と同様、複数の水車120(回転体)を不透過壁10から一定の間隔を空けつつ、平面視において不透過壁10の延びる方向に沿って配列することにより構成される。しかしながら、各水車120は、第1実施形態と異なり、サボニウス水車が上下方向に積層された複数段構成とはなっておらず、一段構成である。しかしながら、第2実施形態のサボニウス水車120を多段構成とすることもできる。
Further, in the
水車120は、上下方向に上から順に、軸上部131、翼部132及び軸下部133を有している。翼部132は、上フランジ134、下フランジ135及び一対の水車翼136を含んでいる。
The
各水車翼136は、半円筒形状であり、水車120は、2枚の水車翼136が水車120の回転軸121に対して180°回転対称に配置されたサボニウス型である。このため、第1実施形態と同様、水車120も、一方向にのみ回転することができる。各水車翼136は、上端部に上フランジ134が連結され、下端部に下フランジ135が連結されており、両フランジ134,135の外周に達しているが、外周から外側へは突出していない。また、水車翼136の上部は、一般的な気象条件下では、常に水面114よりも上方に露出している。軸上部131及び軸下部133は、不透過壁10に対して平行であり、不透過壁10から一定の距離を空けて配置されている。
Each
上フランジ134の上面の中心には、軸上部131の下端部が連結されており、軸上部131と上フランジ134とは同軸である。軸上部131は、鉛直方向に延びており、その上端部が屋根部12に設けられた貫通孔115に挿入され、回転自在に軸支されている。同様に、下フランジ135の下面の中心には、軸下部133の上端部が連結されており軸下部133と下フランジ135とは同軸である。軸下部133は、鉛直方向に延びており、その下端部が底部13の上面に設けられた軸受孔116に挿入され、回転自在に軸支されている。
The lower end portion of the shaft
また、図4に示すように、本実施形態に係る隣り合う2つの水車120も、相反する方向に回転するように構成されている。すなわち、平面視において反時計回りに回転する水車120(以下、第1水車120Aということがある)と、平面視において時計回りに回転する水車(以下、第2水車120Bということがある)とが、水車120の配列方向に沿って交互に配列されている。横断面視において、隣り合う第1水車120Aと第2水車120Bとは、両水車120A,120Bの回転軸121から等距離にある直線に対し、線対称な形状を有している。水車列2の間を波が通過するとき、第1水車120Aの2枚の水車翼136は、いずれも当該第1水車120Aが平面視において反時計回りに回転するように波に押される。同様に、第2水車120Bの2枚の水車翼136も、いずれも当該第2水車120Bが平面視において時計回りに回転するように波に押される。
Moreover, as shown in FIG. 4, the two
以上のとおり、隣り合う水車120A,120Bは、回転方向が逆向きである。このため、隣り合う第1水車120Aの回転軸121と、第2水車120Bの回転軸121との間は、沖側から不透過壁10側に流入しようとする波F1が通過する流入領域118、又は不透過壁側から沖側へ流出しようとする波F2が通過する流出領域119となる。流入領域118と流出領域119とは、水車120の配列方向に沿って交互に形成される。
As described above, the
本実施形態では、第1整流部材150は複数存在して列を形成しており、第2整流部材160も複数存在して列を形成している。第1整流部材150及び第2整流部材160は、各々、鉛直方向に延びており、それぞれの上端部が屋根部12の下面に固定され、それぞれの下端部が底部13の上面に固定されている。第1整流部材150及び第2整流部材160は、直方体形状であり、図4に示すように、横断面(水平方向の断面)形状は正方形である。第1整流部材150及び第2整流部材160の正方形である横断面の対角線の寸法は、水車120の上フランジ134及び下フランジ135の直径とほぼ同じである。
In the present embodiment, a plurality of first rectifying
第1整流部材150は、流出領域119の沖側の近傍に配置され、その横断面の4つの頂点のうちの1つ(以下、第1頂点151という)を流出領域119側に向けている。より詳しくは、第1整流部材150は、横断面視において第1整流部材150の第1頂点151とその対角の第2頂点152とを通る仮想線142が、隣り合う第1水車120A及び第2水車120Bの回転軸121にそれぞれ対応する点を通る仮想線分141の中点又はその近傍を通るように配置されている。仮想線142及び仮想線分141は、直交する。第1頂点151は、仮想線分141より沖側にあるが、第1整流部材150は、隣り合う第1水車120Aと第2水車120Bとの間に形成された隙間に入り込んでいる。
The
第2整流部材160は、流入領域118の不透過壁10側の近傍に配置され、その横断面の4つの頂点のうちの1つ(以下、第1頂点161という)を流入領域118側に向けている。より詳しくは、第2整流部材160は、横断面視において第2整流部材160の第1頂点161とその対角の第2頂点162とを通る仮想線144が、隣り合う第1水車120A及び第2水車120Bの回転軸121にそれぞれ対応する点を通る仮想線分143の中点又はその近傍を通るように配置されている。仮想線144及び仮想線分143は、直交する。第1頂点161は仮想線分143より不透過壁10側にあるが、第2整流部材160は、隣り合う水車120間に形成された隙間に入り込んでいる。
The
次に、この波力発電システム101が波を消波しつつ、発電する仕組みについて説明する。図4に示すように、不透過壁10側に流入しようとする波F1は、流出領域119の下流側に配置された第1整流部材150の沖側に位置する第2頂点152に対応する角部にぶつかり左右(図4における上下方向、以下同じ)に分けられ流入領域118に導かれる。その後、波F1は、第1水車120A及び第2水車120Bの水車翼136の内周面を押して、両水車120A,120Bを回転させる。このとき、平面視において第1水車120Aは反時計回りに回転し、第2水車120Bは時計回りに回転する。波F1は、第1水車120A及び第2水車120Bを回転させた後、流入領域118の下流側に配置された第2整流部材160の沖側に位置する第1頂点161に対応する角部にぶつかり、淀みなく流出領域119へ流入する。
Next, a description will be given of a mechanism in which the wave
また、不透過壁10側から流出しようとする波F2は、流入領域118の下流側に配置された第2整流部材160の不透過壁10側に位置する第2頂点162に対応する角部にぶつかり左右に分けられ、流出領域119に導かれる。その後、波F2は、第1水車120A及び第2水車120Bの水車翼136の内周面を押して、両水車120A,120Bを回転させる。このとき、平面視において第1水車120Aは反時計回りに回転し、第2水車120Bは時計回りに回転する。波F2は、第1水車120A及び第2水車120Bを回転させた後、流出領域119の下流側に配置された第1整流部材150の不透過壁10側に位置する第1頂点151に対応する角部にぶつかり、淀みなく沖側へ流出する。
Further, the wave F <b> 2 about to flow out from the
このように、流入出しようとする波F1,F2の全体は、第1整流部材150及び第2整流部材160によって流入領域118及び流出領域119に導かれ、第1水車120A及び第2水車120Bを一方向に回転させることができる。つまり、この防波堤は、波のエネルギーの多くを水車120の回転エネルギーに変換し、消波することができる。また、波F1,F2は、第1整流部材150及び第2整流部材160により、水車120の水車翼136の内周面に水流を導くが、水車翼136の外周面には水流を導かないため、水車120の回転の抵抗とはならない。
In this way, the entire waves F1 and F2 that are about to flow in and out are guided to the
以上のようにして水車120が回転すると、発電機3は、その回転力を軸上部131を介して受け取り、発電を行う。なお、図3に示すとおり、本実施形態では、発電機3は屋根部12上に配置されているが、第1実施形態と同様に屋根部12の下方に配置されていてもよい。本実施形態でも、第1実施形態と同じく、発電機3の配置及び構成は適宜選択することができる。発電機3で発電された電力は、図示されない送電設備を介して、陸側の変電所等に送電される。なお、図3に示すように、不透過壁10を海岸125に接する又は概ね接するように設置することもできる。
When the
<3.第3実施形態>
次に、第3実施形態に係る波力発電システム201について説明する。図5は、波力発電システム201の横断面図である。波力発電システム201は、第1及び第2実施形態に係る波力発電システム1,101と多くの点で共通する。以下では、第1及び第2実施形態との相違点を中心に説明することとし、第1及び第2実施形態と同様の構成には同様の参照符号を付して詳細な説明を省略する。
<3. Third Embodiment>
Next, a wave
波力発電システム201は、第1及び第2実施形態と同様に、不透過壁10、屋根部12(上壁部)、底部13、土台11、水車列2及び発電機3を備える他、第1整流部材250及び第2整流部材260を備える。本実施形態に係る波力発電システム201と、第2実施形態に係る波力発電システム101との主な相違点は、水車列2に含まれる水車120間の距離にある。
Similar to the first and second embodiments, the wave
より具体的には、本実施形態では、隣り合う第1水車120Aと第2水車120Bとの間を実質的に隙間なく配置している。こうすることで、第1水車120Aと第2水車120Bとの間の隙間を、水車120A,120Bの回転に殆ど寄与することなくすり抜ける波の量を減らすことができる。すなわち、発電効率を向上させることができる。
More specifically, in the present embodiment, the adjacent
本実施形態では、第1整流部材250は、複数存在して列を形成しており、第2整流部材260も、複数存在して列を形成している。第1及び第2整流部材250,260は、第2実施形態に係る第1及び第2整流部材150,160と比較して横断面形状のみが異なり、その余の点においては同様の構成を有する。
In the present embodiment, a plurality of first rectifying
図5に示すように、第1整流部材250の横断面形状は、一対の隣接する曲線253及び一対の隣接する線分254で囲まれた4つの頂点を有する形状である。第1整流部材250は、流出領域119の沖側の近傍に配置され、その横断面の4つの頂点のうちの1つであって一対の曲線253の交点(以下、第1頂点251という)を流出領域119側に向けている。第2頂点252は、一対の線分254の交点である。より詳しくは、第1整流部材250は、横断面視において第1整流部材250の第1頂点251とその対角の第2頂点252とを通る仮想線242が、隣り合う第1水車120A及び第2水車120Bの回転軸121にそれぞれ対応する点を通る仮想線分241の中点又はその近傍を通るように配置されている。また、仮想線242及び仮想線分241は、直交する。第1頂点251は、仮想線分241より沖側にあるが、第1整流部材250は、隣り合う水車120間に形成された隙間に入り込んでいる。第1整流部材250の横断面の4つの頂点のうち、第1頂点251及び第2頂点252ではない残りの頂点間の寸法は、水車120の上フランジ134及び下フランジ135の直径とほぼ同じである。第1整流部材250の横断面において、第1頂点251に対応する角部から左右方向(図5における上下方向、以下同じ。)に延びる曲線253は、水車120の上フランジ134及び下フランジ135と同心で、僅かに径の大きい円弧状である。
As shown in FIG. 5, the cross-sectional shape of the
第2整流部材260の横断面形状は、一対の隣接する曲線263及び一対の隣接する線分264で囲まれた4つの頂点を有する形状である。第2整流部材260は、流入領域118の不透過壁10側の近傍に配置され、その横断面の4つの頂点のうちの1つであって一対の曲線263の交点(以下、第1頂点261という)を流入領域118側に向けている。第2頂点262は、一対の線分264の交点である。より詳しくは、第2整流部材260は、横断面視において第2整流部材260の第1頂点261とその対角の第2頂点262とを通る仮想線244が、隣り合う第1水車120A及び第2水車120Bの回転軸121にそれぞれ対応する点を通る仮想線分243の中点又はその近傍を通るように配置されている。また、仮想線244及び仮想線分243は、直交する。第1頂点261は、仮想線分243より不透過壁10側にあるが、第2整流部材260は、隣り合う水車120間に形成された隙間に入り込んでいる。第2整流部材260の横断面の4つの頂点のうち、第1頂点261及び第2頂点262ではない残りの頂点間の寸法は、水車120の上フランジ134及び下フランジ135の直径とほぼ同じである。第2整流部材260の横断面において、第1頂点261に対応する角部から左右方向(図5における上下方向、以下同じ。)に延びる曲線263は、水車120の上フランジ134及び下フランジ135と同心で、僅かに径の大きい円弧状である。
The cross-sectional shape of the
以上の構成により、第3実施形態に係る波力発電システム201では、既に述べた波力発電システム1,101よりも発電効率を向上させることができる。
With the above configuration, the wave
<4.第4実施形態>
次に、第4実施形態に係る波力発電システム301について説明する。図6は、波力発電システム301の横断面図である。波力発電システム301は、第1~第3実施形態に係る波力発電システム1,101,201と多くの点で共通する。以下では、第1~第3実施形態との相違点を中心に説明することとし、第1~第3実施形態と同様の構成には同様の参照符号を付して詳細な説明を省略する。
<4. Fourth Embodiment>
Next, a wave
波力発電システム301は、第1~第3実施形態と同様に、不透過壁10、屋根部12(上壁部)、底部13、土台11、水車列2及び発電機3を備える他、第1整流部材350及び第2整流部材360を備える。本実施形態に係る波力発電システム301と、第2及び第3実施形態に係る波力発電システム101,202との主な相違点は、水車列2に含まれる水車120間の距離にある。
Similar to the first to third embodiments, the wave
より具体的には、波力発電システム301では、水車列2に含まれる水車120が、不等間隔で配列されている。特に、本実施形態では、水車列2に含まれる水車120は、流入領域118に対応する箇所と流出領域119に対応する箇所とで、異なる間隔を空けて配列されている。流出領域119に対応する位置での隣り合う水車120間の間隔が、流入領域118に対応する位置での隣り合う水車120間の間隔よりも広いが、図7に示すように逆にすることも可能である。
More specifically, in the wave
本実施形態では、防波堤が不透過壁10の沖側に透過性の前壁を有さないため、水車120の設置位置の自由度が高い。従って、発電効率を向上させるような防波堤への波の流入量及び流出量を設置場所ごとに判断し、それに併せて、水車列2に含まれる隣り合う水車120間の各間隔を別々に設定することができる。特に、流入領域118に対応する位置での間隔と、流出領域119に対応する位置での間隔とを別々に設定できることは有意義である。
In the present embodiment, since the breakwater does not have a permeable front wall on the offshore side of the
<5.変形例>
以上、本発明の一実施形態について説明したが、本発明は上記実施形態に限定されるものではなく、その趣旨を逸脱しない限りにおいて、種々の変更が可能である。例えば、以下の変更が可能である。また、以下の変形例の要旨は、適宜組み合わせることができる。
<5. Modification>
As mentioned above, although one Embodiment of this invention was described, this invention is not limited to the said embodiment, A various change is possible unless it deviates from the meaning. For example, the following changes can be made. Moreover, the gist of the following modifications can be combined as appropriate.
<5-1>
上記実施形態では、回転体としてサボニウス水車が用いられたが、これに限られず、他の種類の水車を用いることもできる。ただし、発電効率の観点からは、寄せ波時においても引き波時においても容易に発電が可能なように、波の方向によらず一定の方向に回転する水車を用いることが好ましい。このような水車の例としては、サボニウス水車の他には、クロスフロー水車が挙げられる。また、上記実施形態の水車において、3枚、4枚等の異なる枚数の水車翼を有するように変形した水車を用いることもできる。
<5-1>
In the above embodiment, a Savonius turbine is used as the rotating body, but the present invention is not limited to this, and other types of turbines can also be used. However, from the viewpoint of power generation efficiency, it is preferable to use a water turbine that rotates in a certain direction regardless of the direction of the waves so that power generation can be easily performed at the time of spilling and at the time of wave drawing. As an example of such a water wheel, there is a cross flow water wheel in addition to the Savonius water wheel. Further, in the water wheel of the above embodiment, a water wheel deformed so as to have a different number of water wheel blades such as three or four can be used.
<5-2>
上記実施形態では、水車列2が互い違い回転構成とされたが、これに限定されず、例えば、全ての水車20が同じ方向に回転するように構成してもよい。
<5-2>
In the said embodiment, although the water turbine row |
<5-3>
上記実施形態では、水車の回転軸の上下が軸支されたが、上だけ又は下だけ軸支してもよい。
<5-3>
In the above-described embodiment, the upper and lower sides of the rotating shaft of the water turbine are pivotally supported.
<5-4>
上記実施形態では、水車の回転軸は、直接発電機に連結されたが、例えば、油圧ポンプ等の他の機器を介して間接的に発電機に連結するようにしてもよい。
<5-4>
In the said embodiment, although the rotating shaft of the water turbine was directly connected with the generator, you may make it connect with a generator indirectly through other apparatuses, such as a hydraulic pump, for example.
<5-5>
第2から第4実施形態では、回転軸が中央の翼部の上と下に分かれて配置されたが、翼部132を貫通していてもよい。
<5-5>
In the second to fourth embodiments, the rotation shaft is arranged separately above and below the central wing, but may pass through the
<5-6>
第2から第4実施形態では、翼部132の上部は水面より上方に露出していたが、常に水没させるようにしてもよい。
<5-6>
In the second to fourth embodiments, the upper part of the
<5-7>
上記実施形態では、波力発電システムが海に設置されたが、川や湖等に設置することもできる。
<5-7>
In the above embodiment, the wave power generation system is installed in the sea, but it can also be installed in a river or a lake.
<5-8>
第2から第4実施形態において、第1整流部材及び第2整流部材の一方を省略してもよい。
<5-8>
In the second to fourth embodiments, one of the first rectifying member and the second rectifying member may be omitted.
<5-9>
上記実施形態では、土台11の沖側は、鉛直方向に対し斜面を形成するように構成されていた。しかしながら、図8に示すように、土台11に代えて、沖側に鉛直面111Aを有する土台11Aを設けてもよい。また、図9に示すように、土台11上に設けられた底部13上にさらに土台11Bを形成してもよい。図9の土台11Bは、概ね水車20の下方にのみ形成されており、縦断面視において不透過壁10にまで達していない直方体状の土台であるが、この土台11Bを不透過壁10まで達している土台とすることもできる。なお、本変形例のように、土台を縦断面視において図1のように台形型ではなく、長方形型とした場合には、水車20の直下でありかつ沖側の近傍で急激に水深が変化する段差が形成され、流入してくる波の波長が変化し流速が速くなる。従って、この場合には、波の反射率を低下させる効果及び発電効率を向上させる効果の向上が期待される。
<5-9>
In the said embodiment, the offshore side of the
以下、本発明の実施例1について説明する。但し、本発明は、以下の実施例1に限定されない。 Hereinafter, Example 1 of the present invention will be described. However, the present invention is not limited to the following Example 1.
<1.実験条件>
ここでは、実施例1として、造波水槽を用い、図10に示すような波力発電システムを作成した。具体的に説明すると、造波水槽のサイズは、長さ20.00m、幅0.50m、高さ0.50mとし、水深h=0.40mで一定とした。造波水槽の長さ方向の一端側(沖側)に造波板を設置し、造波板から他端側(岸側)に13.68m離れた位置に水車の回転軸が位置するように、水車列を設置した。水車列に含まれる各水車は、第1実施形態で説明したのと同様の三段構成のサボニウス水車とした。なお、水車列は3種類用意し、各水車列のサボニウス水車の径Ds[m]を、Ds=0.084,0.140,0.210とした。水車列に含まれる水車数は、造波水槽との幅との関係で、Ds=0.084の場合、5つ(図11A参照)、Ds=0.140の場合、3つ(図11B参照)、Ds=0.210の場合2つ(図11C参照)とした。いずれの水車列についても、互い違い回転構成とした。水車間距離D=Ds+2a(2aは、隣接する水車の翼端間距離)は、2a/D=0.11(一定)となるように設定し、水車高さHwは、Hw/hが概ね0.8で一定となるように設定した。また、水車列からさらにl[m]=0.38岸側に、不透過壁を設置した。
<1. Experimental conditions>
Here, as Example 1, a wave power generation system as shown in FIG. Specifically, the size of the wave-making water tank is 20.00 m in length, 0.50 m in width, 0.50 m in height, and constant at a water depth h = 0.40 m. Install a wave plate on one end side (offshore side) in the length direction of the wave tank, so that the rotating shaft of the turbine is located 13.68 m away from the wave plate on the other side (shore side) A watermill was installed. Each turbine included in the turbine train is a Savonius turbine having a three-stage configuration similar to that described in the first embodiment. Three types of water turbine trains were prepared, and the diameter D s [m] of the Savonius turbine in each turbine train was set to D s = 0.084, 0.140, 0.210. The number of turbines included in the turbine wheel row is 5 (see FIG. 11A) when D s = 0.084, and 3 when D s = 0.140 (see FIG. 11) in relation to the width of the wave tank. 11B), and when D s = 0.210, two (see FIG. 11C). All the water turbine trains have a staggered rotation configuration. The distance between the turbines D = D s + 2a (2a is the distance between the blade tips of adjacent turbine wheels) is set to 2a / D = 0.11 (constant), and the turbine height H w is H w / h was set to be approximately constant at 0.8. Further, an impermeable wall was further installed on the shore side of l [m] = 0.38 from the water wheel train.
また、実施例1に係る波力発電システムでは、発電機の代わりに、図12に示す動力計測システムを設置した。水車の回転軸(水車軸)は、ボールベアリング軸受けを用いて、摩擦が極力少なくなるようにその下端を支持した。水車軸の上端は、磁気ブレーキと連結し、当該磁気ブレーキにより水車軸に負荷トルクTq[N・m]を与えた。磁気ブレーキとしては、日本創販株式会社製のPerma-Tork HC01-1を使用した。また、水車軸に加速度計を固定し、サンプリング周波数100Hzで造波開始後30秒~80秒の間、水車の回転速度(角速度)RE[rps]を測定した。また、水車軸から約3.5m沖側に2本の容量式波高計を設置し、水位変動を測定した。また、水車軸から0.18m沖側に1本の容量式波高計を設置し、水車列近傍の水位変動を測定した。波高計のサンプリング周波数はいずれも100Hzとした。作用波は、周期T[s]=0.81~1.67で、波形勾配H/L=0.01の規則波とした。なお、Hは、波高であり、Lは、波長である。 Moreover, in the wave power generation system which concerns on Example 1, the power measurement system shown in FIG. 12 was installed instead of the generator. The rotating shaft of the water turbine (water turbine shaft) was supported at its lower end by using a ball bearing bearing so that friction was minimized. The upper end of the water wheel axis is connected to the magnetic brake, the water axle gave load torque T q [N · m] by the magnetic brake. As the magnetic brake, Perma-Tork HC01-1 manufactured by Nippon Sohatsu Co., Ltd. was used. In addition, an accelerometer was fixed to the turbine shaft, and the rotation speed (angular velocity) R E [rps] of the turbine was measured for 30 to 80 seconds after the start of wave formation at a sampling frequency of 100 Hz. In addition, two capacitive wave height meters were installed approximately 3.5 m offshore from the water wheel shaft, and the water level fluctuation was measured. In addition, one capacitive wave height meter was installed 0.18 m offshore from the water wheel shaft, and the water level fluctuation near the water wheel train was measured. The sampling frequency of the wave height meter was 100 Hz. The working wave was a regular wave with a period T [s] = 0.81 to 1.67 and a waveform gradient H / L = 0.01. Note that H is the wave height and L is the wavelength.
<2.実験結果及び評価>
<2-1.反射率>
Tq=1.1×10-3N・mの場合の反射率Krは、図13A~図13Cに「点」で示される結果となった。図13A~図13Cは、それぞれDs/h=0.215、0.350、0.525の場合のデータを示している。なお、反射率Krは、水車列から約3.5m沖側の2本の容量式波高計による測定結果に基づいて、入・反射波分離推定法(合田ら,1976年,不規則波における入・反射波の分離推定法,港湾技術研究所資料,No.248)を用いて算出した。また、水車列の代わりに、円柱列を用いた場合(他の条件は、上述の実施例1と同じ)の縦スリット直立消波工のモデル(比較例)を想定し、当該比較例での反射率Krを既往研究による理論解として算出したところ、図13A~図13Cに「曲線」で示される結果となった。なお、当該比較列における円柱列は、上述の水車列と同じ径の円柱を同じ間隔で配列したものである。
<2. Experimental results and evaluation>
<2-1. Reflectivity>
T q = 1.1 reflectance K r in the case of × 10 -3 N · m has resulted represented by "dots" in FIGS. 13A ~ FIG 13C. 13A to 13C show data when D s /h=0.215, 0.350, and 0.525, respectively. The reflectivity K r is calculated based on the measurement results of two capacitive wave height meters approximately 3.5 m offshore from the turbine wheel train. This was calculated using the separation / estimation method of incoming and reflected waves, Port Technology Institute data, No. 248). Further, assuming a model (comparative example) of a vertical slit upright wave breaker when a columnar column is used instead of a turbine row (other conditions are the same as those of the first embodiment described above), When the reflectance K r was calculated as a theoretical solution based on previous studies, the results shown by “curves” in FIGS. 13A to 13C were obtained. Note that the column column in the comparison column is a column in which columns having the same diameter as the above-described turbine column are arranged at the same interval.
図13A~図13Cからは、実施例1においては比較例よりも、反射率Krが低くなる傾向にあることが分かる。この傾向は、特に短周期側で顕著であった。これは、水流が水面下に存在する水車の上面を通過することでより大きなせん断流が発生し、エネルギーを損失しているからと考えられる。また、水車の径Dsが大きい程、水車上面の面積が大きくなり、より多くの波のエネルギーを消散し、反射率Krの低減につながっていると考えられる。すなわち、透過性の前壁を設置せずとも、水車列により十分に消波を行うことができることが分かった。また、海域の静穏性を保つためには、水車の径を水深及び波浪の周期に応じて決定すればよいことが分かった。また、水車の径を水深の20%~50%程度とした場合において、30%~80%程度の反射率を実現することが可能であり、特に、水車の径を水深の50%程度とした場合において、30%~50%程度の反射率を実現することが可能である。 From FIG. 13A to FIG. 13C, it can be seen that the reflectance K r tends to be lower in Example 1 than in the comparative example. This tendency was particularly remarkable on the short cycle side. This is presumably because a larger shear flow is generated by passing through the upper surface of the water wheel existing below the water surface and energy is lost. In addition, it is considered that the larger the diameter D s of the turbine wheel, the larger the area of the upper surface of the turbine wheel, so that more wave energy is dissipated and the reflectance K r is reduced. In other words, it was found that the water turbine train can be sufficiently extinguished without installing a permeable front wall. Moreover, in order to maintain the calmness of the sea area, it was found that the diameter of the water wheel should be determined according to the water depth and the wave period. Further, when the diameter of the water wheel is set to about 20% to 50% of the water depth, it is possible to realize a reflectance of about 30% to 80%. In particular, the diameter of the water wheel is set to about 50% of the water depth. In some cases, a reflectivity of about 30% to 50% can be achieved.
また、上記実施形態に係る波力発電システムでは、水車軸に発電機が取り付けられているため、この発電機により水車軸に負荷(ブレーキ)が掛かり、水車軸の回転速度が小さくなると予想される。そこで、この影響を評価するため、様々な負荷トルクTqに対する回転速度RE及び反射率Krを測定したところ、図14A~図14Cに示す結果が得られた。図14A~図14Cは、それぞれDs/h=0.215、0.350、0.525の場合のデータを示している。 Further, in the wave power generation system according to the above embodiment, since the generator is attached to the water wheel shaft, it is expected that a load (brake) is applied to the water wheel shaft by this power generator, and the rotation speed of the water wheel shaft is reduced. . Therefore, in order to evaluate this influence, the rotational speed R E and the reflectance K r with respect to various load torques T q were measured, and the results shown in FIGS. 14A to 14C were obtained. 14A to 14C show data when D s /h=0.215, 0.350, and 0.525, respectively.
図14A~図14Cからは、負荷トルクTqの増加とともに、回転速度REは減少するが、反射率Krには有意な変化が見られないことが分かる。すなわち、反射率は、発電機の負荷に影響を受けず、構造条件(水深、水車の径、周期、波長等の波浪条件)等に応じて決定されることが分かった。また、発電機の負荷によらず反射率が一定であることから、水車周りに形成される渦の発生により消散されるエネルギー量と、水車を回転させるために使用されるエネルギー量とからなるエネルギーの総消散量は、発電機の負荷によらず一定となることが分かった。 From FIG. 14A to FIG. 14C, it can be seen that as the load torque T q increases, the rotational speed RE decreases, but no significant change is observed in the reflectance K r . That is, it has been found that the reflectivity is not affected by the load of the generator and is determined according to the structural conditions (wave conditions such as water depth, water wheel diameter, period, wavelength, etc.). In addition, since the reflectance is constant regardless of the load on the generator, energy consisting of the amount of energy dissipated by the generation of vortices formed around the turbine and the amount of energy used to rotate the turbine It was found that the total dissipated amount was constant regardless of the generator load.
<2-2.獲得動力>
様々な水車の径Dsに対する獲得動力効率Keを、以下の式に従って算出したところ、図15A~図15Cに示す結果が得られた。図15A~図15Cは、それぞれDs/h=0.215、0.350、0.525の場合のデータを示している。以下のPpは、水車の回転により得られた単位幅あたりの獲得動力であり、Pwは、単位幅当たりの波のエネルギーである。なお、ρは、水の密度であり、gは、重力加速度である。また、以下の式中のREは、平均回転速度である。
Acquisition power efficiency K e to the diameter D s of different waterwheel, was calculated according to the following equation, the results shown in FIGS. 15A ~ FIG 15C is obtained. 15A to 15C show data when D s /h=0.215, 0.350, and 0.525, respectively. P p below is the acquired power per unit width obtained by the rotation of the water turbine, and P w is the wave energy per unit width. Note that ρ is the density of water and g is the acceleration of gravity. Further, R E in the following formula is an average rotation speed.
既往研究によると、サボニウス水車による波のエネルギーを対象とした発電効率(獲得動力効率)は、5%程度であるとされている。一方、実施例1に係る波力発電システムでは、図15A~図15Cに示すとおり、いずれの水車の径Dsに対しても、獲得動力効率Keの最大値は10%以上となり、高い発電効率が期待されることが分かった。 According to previous studies, the power generation efficiency (acquired power efficiency) for wave energy generated by Savonius turbines is about 5%. Meanwhile, in the wave activated power generation system according to the first embodiment, as shown in FIGS. 15A ~ FIG 15C, even for the diameter D s of any hydraulic turbine, the maximum value of the acquired power efficiency K e becomes 10% or more, high power It turns out that efficiency is expected.
また、発電の安定性の観点からは、水車の回転速度の変動が少ないことが求められる。そこで、水車軸から0.18m沖側での推移変動ηと、水車の回転速度REとの関係を調べたところ、図16A~図16Cに示す結果が得られた。図16A~図16Cは、それぞれDs/h=0.215、0.350、0.525の場合のデータを示している。 In addition, from the viewpoint of power generation stability, it is required that fluctuations in the rotational speed of the water turbine be small. Therefore, the transition varies η at 0.18m offshore water axle, was examined the relationship between the rotational speed R E of the water wheel, the results shown in FIGS. 16A ~ FIG 16C is obtained. 16A to 16C show data when D s /h=0.215, 0.350, and 0.525, respectively.
図16Aに示すとおり、Ds/h=0.215の場合には、1波に対して2回の回転速度のピークが現れた。このような傾向は、回転速度は入射波が水車列を通過する際に増大し、不透過壁で反射した反射波が沖側に伝播してゆく際に再び増大することによるものと考えられる。また、図16B及び図16Cに示すとおり、Ds/hが0.350,0.525と大きくなるにつれて、回転速度REの変動は小さくなった。すなわち、水車の径が大きいと、水車が一度周り始めた後は慣性モーメントが作用して波の周波特性を受けにくくなり、安定した速度で回転するようになると考えられる。従って、発電の安定性の観点からは、水車の径が大きい方が有利であると言え、水車の径は、水深の30%以上のサイズとすることが好ましく、特に50%以上のサイズとすることが好ましいことが分かった。 As shown in FIG. 16A, in the case of D s /h=0.215, two rotation speed peaks appeared for one wave. Such a tendency is considered to be due to the fact that the rotational speed increases when the incident wave passes through the water wheel train and increases again when the reflected wave reflected by the non-transparent wall propagates offshore. Further, as shown in FIGS. 16B and 16C, as D s / h is increased and 0.350,0.525, variation of the rotational speed R E was smaller. That is, if the diameter of the water wheel is large, it is considered that after the water wheel starts to rotate once, the moment of inertia acts to make it difficult to receive the frequency characteristic of the wave, and the water wheel rotates at a stable speed. Therefore, it can be said that the larger diameter of the water turbine is more advantageous from the viewpoint of the stability of power generation, and the diameter of the water turbine is preferably 30% or more of the water depth, particularly 50% or more. It turned out to be preferable.
以下、本発明の実施例2について説明する。但し、本発明は、以下の実施例2に限定されない。 Hereinafter, Example 2 of the present invention will be described. However, the present invention is not limited to the following Example 2.
<1.実験条件>
ここでは、実施例2として、造波水槽を用い、図17、図18A及び図18Bに示すような波力発電システムを作成した。具体的に説明すると、造波水槽のサイズは、長さ20.00m、幅0.50m、高さ0.60mとし、最大水深h=0.40mで一定とした。造波水槽の長さ方向の一端側(沖側)に造波板を設置し、造波板から他端側(岸側)に約14m離れた位置に水車列の回転軸を設置した。また、水車列の回転軸からさらにl[m]岸側に、不透過壁を設置した。サボニウス水車の径Ds[m]=0.072とした。水車列に含まれる水車数は、6つとし、水車列を、隣接する水車が逆回転する互い違い回転構成とした。また、水車間距離D[m]=1.1Dsとした。水車列に含まれる各水車は、第1実施形態で説明した三段構成のサボニウス水車を二段構成に変更した構成とした。また、不透過壁から沖側にl’[m]広がり、幅方向には造波水槽の幅だけ広がる直方体のステップ11Aを用意し、当該ステップ11A上に水車列を配置した。
<1. Experimental conditions>
Here, as Example 2, a wave power generation system as shown in FIGS. 17, 18 </ b> A, and 18 </ b> B was created using a wave-making water tank. Specifically, the size of the wave water tank is 20.00 m in length, 0.50 m in width, 0.60 m in height, and constant at a maximum water depth h = 0.40 m. A wave-making plate was installed on one end side (offshore side) of the wave-making water tank in the length direction, and a rotating shaft of the water wheel train was installed at a position about 14 m away from the wave-making plate on the other end side (shore side). In addition, an impermeable wall was installed on the l [m] shore side further from the rotation axis of the water wheel train. The diameter D s [m] of the Savonius turbine was set to 0.072. The number of water turbines included in the water turbine train is six, and the water turbine train has a staggered rotation configuration in which adjacent water turbines rotate in reverse. In addition, a water wheel distance D [m] = 1.1D s. Each turbine included in the turbine row is configured by changing the three-stage Savonius turbine described in the first embodiment to a two-stage configuration. In addition, a
また、実施例2に係る波力発電システムでは、発電機の代わりに、図12と同様の動力計測システムを設置し、水車軸に負荷トルクTq[N・m]を与えた。また、水車間(沖側)かつ静水面下0.08mの位置に、アレック電子社製の電磁流速計を設置し、水車間の流速を計測した。また、水車軸の上端に取り付けたATRプロモーションズ株式会社製の加速度計(センサーコントローラ)を用いて、水車の回転速度ωをサンプリング周波数100Hzで計測した。さらに、水車の回転軸から約3.5m沖側に2本の容量式波高計を設置し、入・反射波分離推定法(合田ら,1976年,不規則波における入・反射波の分離推定法,港湾技術研究所資料,No.248)を用いて、入射波の波高H[m]及び反射率Krを求めた。また、水車一本に作用する波エネルギーD・Pω(Pω=ρgH2/8)に対する水車の獲得動力Pの比として求められる一次変換効率Eを求め、これを水車の単位長さ当たりに換算したエネルギー変換効率E’=E/Hsを求めた。なお、Hs[m]は、水車の高さである。作用波は、周期T[s]=0.73~1.71で、波形勾配H/L=0.020の規則波とした。なお、Hは、波高であり、Lは、波長である。 In the wave power generation system according to Example 2, a power measurement system similar to that shown in FIG. 12 was installed instead of the generator, and a load torque T q [N · m] was applied to the water wheel shaft. In addition, an electromagnetic current meter made by Alec Electronics Co., Ltd. was installed at a position between the turbines (offshore) and 0.08 m below the static water surface, and the flow velocity between the turbines was measured. Further, the rotational speed ω of the water turbine was measured at a sampling frequency of 100 Hz using an accelerometer (sensor controller) manufactured by ATR Promotions Inc. attached to the upper end of the water wheel shaft. In addition, two capacitive wave height meters were installed approximately 3.5 m offshore from the rotating shaft of the turbine, and separate input / reflected wave estimation method (Goda et al., 1976, separate estimation of incoming / reflected wave in irregular waves). Law, Port Technology Research Institute, No. 248), the wave height H [m] and the reflectance K r of the incident wave were obtained. Also, determine the primary conversion efficiency E obtained as the ratio of the acquired power P hydraulic turbine for wave energy D · Pω acting on one water turbine (Pω = ρgH 2/8) , which was converted to per unit length of the waterwheel The energy conversion efficiency E ′ = E / H s was determined. H s [m] is the height of the water wheel. The working wave was a regular wave having a period T [s] = 0.73 to 1.71 and a waveform gradient H / L = 0.020. Note that H is the wave height and L is the wavelength.
そして、ステップ11Aのみの条件下(case1:比較例)と、水車列のみの条件下(case2:実施例)と、図17に示すステップ11A及び水車列の両方を用意した条件下(case3:実施例)において、l’=l+0.04とし、l=0.20m,0.30m,0.40mと変化させながら実験を行った。さらに、l’=0.44(一定)として、l/l’を変化させて実験を行った。なお、case1の波力発電システムは、図17の波力発電システムから水車列を除去したものである。また、case2の波力発電システムは、図17の波力発電システムからステップ11Aを除去し、二段構成の水車列を三段構成に変更したものである。case1~case3でのhs/h及び水車の高さHsに関する実験条件は、下表のとおりである。なお、hs[m]は、水車の設置位置での水深である。
<2.実験結果及び評価>
ステップ長(岸-沖方向のステップ11Aの長さ)l’をl’=0.24,0.34,0.44mと変化させた場合の、反射率Krおよび水車間を通過する最大流速Vmax(ステップ11Aのみの場合には、水車の設置位置における計測値)は、それぞれ図19A~図19Cに示すとおりの結果となった。図中のumaxは,水深h=0.40mにおける微小振幅波理論から求められる最大速度振幅を表している。同図からは、ステップ11Aのみのcase1では、概して反射率Krは0.6以上と高い傾向にあることが分かった。水車列のみのcase2は,いずれのl’条件下においても、case1よりも反射率が低いことが分かった。さらに、ステップ11A上に水車列を設けたcase3では、短周期帯においてはcase2とほぼ同じKrとなっているが、長周期帯においては大幅なKrの低下傾向が見られ、ステップ11Aが長い程この傾向が顕著であることが分かった。一方、case3のVmax/umaxは、case2のそれよりも大きい。従って、ステップ11A上に水車を設置することにより、水車間を通過する流速が速くなりエネルギー散逸が大きくなって、反射率Krが低下したと考えられる。
<2. Experimental results and evaluation>
Step length - in the case of 'a l' (shore offshore length in the direction of the
以上より、反射率Krは、case3で最も低く、case2で次に低く、case1で最大になる傾向が確認された。従って、水車列により消波性能が向上し、さらに水車列をステップ11A上に設置した場合には、消波性能がさらに向上することが確認された。
From the above, it was confirmed that the reflectivity Kr tends to be the lowest in
図20A及び図20Bは、ステップ長l’=0.44(一定)にして負荷トルクTqを与えたときの、それぞれcase2およびcase3のエネルギー変換効率E’を示している。同図より、case3でのE’の極大値は0.6程度であり、case2では0.4程度であり、case3での方がcase2の場合よりも、概してエネルギー変換効率E’が高いことが分かった。従って、水車列をステップ11A上に設置することで、発電効率が向上することが分かった。より詳細には、ステップ11Aを設けたうえで水車列を設置した場合、概ねエネルギー変換効率E’が向上するとともに、いずれの周期の波に対してもほぼ一定の負荷トルク(Tq=0.003N・m程度)で最大エネルギー変換効率を取ることが分かった。このことは、効率良くエネルギーを獲得するための最適負荷トルクが、対象の波の周期にかかわらず一定であることを意味し、二次変換機構(発電機等を作動させるための機構)の設計においては有用な知見が得られていると言える。
20A and 20B show the energy conversion efficiencies E ′ of
図21は、ステップ長l’=0.44(一定)の条件下で、l/l’=0.45,0.68,0.91と変化させたときの、反射率Kr及び水車間を通過する最大流速Vmaxとを示している。同図からは、l/l’が大きくなるほど、すなわち、水車列の設置位置がステップ11Aの沖側になるほどKrの極小値が小さくなる傾向があることが確認された。従って、消波の観点からは、水車列は、ステップ11Aの沖側端の近傍に配列することが好ましいことが分かった。
FIG. 21 shows the reflectance K r and the distance between the water wheels when the length is changed to 1 / l ′ = 0.45, 0.68, 0.91 under the condition of the step length l ′ = 0.44 (constant). The maximum flow velocity Vmax passing through is shown. From the figure, the larger the l / l ', i.e., that there is a tendency that the minimum value of about K r installation position of the water wheel column is
図22A及び図22Bは、それぞれl/l’=0.91,0.45の場合の一次変換効率Eを示している。同図からは、l/l’が大きくなるほど、すなわち、水車列の設置位置がステップ11Aの沖側になるほど、一次変換効率Eの極大値が大きくなる傾向があることが確認された。従って、発電効率の観点からも、水車列は、ステップ11Aの沖側端の近傍に配列することが好ましいことが分かった。
22A and 22B show the primary conversion efficiency E when l / l ′ = 0.91 and 0.45, respectively. From the figure, it was confirmed that the maximum value of the primary conversion efficiency E tends to increase as l / l ′ increases, that is, as the installation position of the water turbine row is on the offshore side of
1,101,201,301 波力発電システム
2 水車列(回転体列)
3 発電機
10 不透過壁
11,11A,11B 土台(ステップ)
12 屋根部(上壁部)20,120 水車(回転体)
120A 第1水車
120B 第2水車
21,121 回転軸
118 流入領域
119 流出領域
150,250,350 第1整流部材
160,260,360 第2整流部材
1, 101, 201, 301 Wave
3
12 Roof part (upper wall part) 20,120 Water wheel (rotary body)
120A
Claims (12)
前記不透過壁の沖側において、平面視において前記不透過壁の延びる方向に沿って配列された複数の回転体からなる回転体列と、
前記複数の回転体の回転エネルギーを電力に変換する発電機と
を備える、波力発電システム。 It is installed in water and has an impermeable wall, but is used with a breakwater that does not have a permeable front wall on the offshore side of the impermeable wall, dissipates wave energy, and generates electricity from the wave energy. A wave power generation system,
On the offshore side of the impermeable wall, a rotating body row composed of a plurality of rotating bodies arranged along a direction in which the impermeable wall extends in a plan view;
A wave power generation system comprising: a generator that converts rotational energy of the plurality of rotating bodies into electric power.
請求項1に記載の波力発電システム。 The adjacent rotating bodies included in the rotating body row are configured to rotate in opposite directions.
The wave power generation system according to claim 1.
前記流入領域及び前記流出領域は、各々少なくとも1つ形成され、
前記流出領域の沖側の近傍に配置され、沖側から前記不透過壁側に流入する波を前記流入領域に導く第1整流部材、及び、前記流入領域の前記不透過壁側の近傍に配置され、前記不透過壁側から沖側へ流出する波を前記流出領域に導く第2整流部材の少なくとも一方
をさらに備える、
請求項1又は2に記載の波力発電システム。 Between the rotating shafts of adjacent rotating bodies included in the rotating body row, an inflow region where waves flowing from the offshore side to the impermeable wall side pass, or waves flowing out from the impermeable wall side to the offshore side pass. The outflow area
At least one of the inflow region and the outflow region is formed,
A first rectifying member that is disposed near the outflow region on the offshore side and guides waves flowing from the offshore side to the impermeable wall side to the inflow region, and disposed near the impermeable wall side of the inflow region And further comprising at least one second rectifying member for guiding the wave flowing out from the impermeable wall side to the offshore side to the outflow region,
The wave power generation system according to claim 1 or 2.
請求項3に記載の波力発電システム。 The rotating bodies included in the rotating body row are arranged at different intervals at a position corresponding to the inflow area and a position corresponding to the outflow area,
The wave power generation system according to claim 3.
請求項1から4のいずれかに記載の波力発電システム。 The rotating bodies included in the rotating body row are arranged at unequal intervals.
The wave power generation system according to any one of claims 1 to 4.
をさらに備える、
請求項1から5のいずれかに記載の波力発電システム。 Further comprising an upper wall portion extending in a horizontal direction from the impermeable wall and supporting the rotating body;
The wave power generation system according to any one of claims 1 to 5.
をさらに備える、
請求項1から5のいずれかに記載の波力発電システム。 A caisson having the impervious wall, and a bottom part and an upper wall part extending from the lower and upper parts of the impervious wall to the offshore side, respectively.
The wave power generation system according to any one of claims 1 to 5.
をさらに備える、
請求項1から7のいずれかに記載の波力発電システム。 The foundation in which the rotating body row is installed, and the water depth at the installation location of the rotating body row is shallower than the water depth at the offshore side,
Further comprising
The wave power generation system according to any one of claims 1 to 7.
請求項8に記載の波力発電システム。 The foundation has a vertical surface facing the offshore side,
The wave power generation system according to claim 8.
請求項1から9のいずれかに記載の波力発電システム。 The rotating body is a water wheel that rotates in a constant direction regardless of the direction of the waves.
The wave power generation system according to any one of claims 1 to 9.
請求項10に記載の波力発電システム。 The rotating body is a Savonius turbine.
The wave power generation system according to claim 10.
請求項1から11のいずれかに記載の波力発電システム。 The rotating shaft of the rotating body extends in the vertical direction.
The wave power generation system according to any one of claims 1 to 11.
Priority Applications (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201580012183.1A CN106103977A (en) | 2014-06-12 | 2015-05-28 | Wave power generation system |
| JP2016527735A JPWO2015190297A1 (en) | 2014-06-12 | 2015-05-28 | Wave power generation system |
| KR1020167037080A KR20170020385A (en) | 2014-06-12 | 2015-05-28 | Wave-activated power generation system |
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| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2014121120 | 2014-06-12 | ||
| JP2014-121120 | 2014-06-12 |
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| WO2015190297A1 true WO2015190297A1 (en) | 2015-12-17 |
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| PCT/JP2015/065343 Ceased WO2015190297A1 (en) | 2014-06-12 | 2015-05-28 | Wave-activated power generation system |
Country Status (5)
| Country | Link |
|---|---|
| JP (1) | JPWO2015190297A1 (en) |
| KR (1) | KR20170020385A (en) |
| CN (1) | CN106103977A (en) |
| TW (1) | TWI638096B (en) |
| WO (1) | WO2015190297A1 (en) |
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| CN106908216A (en) * | 2017-02-22 | 2017-06-30 | 哈尔滨工程大学 | A kind of ship model experimental tank wave absorber |
| KR102162039B1 (en) * | 2020-05-19 | 2020-10-06 | 주식회사 그린월 | Falling type wall and construction method thereof |
Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58214678A (en) * | 1982-06-07 | 1983-12-13 | Mitsubishi Heavy Ind Ltd | Collective device of wave energy |
| US20080088132A1 (en) * | 2006-10-17 | 2008-04-17 | Laube Von Laubenfels Walter He | Wave rider |
| JP2013209978A (en) * | 2012-02-29 | 2013-10-10 | Kyb Co Ltd | Wave power generator |
Family Cites Families (14)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5224643A (en) * | 1975-04-25 | 1977-02-24 | Chiyuuka Nougen Kaihatsu Kofun | Energy convertor for wave * ocean current or tide and the like |
| JPS5644466A (en) * | 1979-09-20 | 1981-04-23 | Muroran Kogyo Daigaku | Wave energy absorptive device installed to for breakwater |
| JPS5928070A (en) * | 1982-08-09 | 1984-02-14 | Mitsubishi Electric Corp | Wave force-to-energy converter |
| CN2151270Y (en) * | 1992-11-30 | 1993-12-29 | 刘百清 | Wave breakwater power generation device |
| US5461862A (en) * | 1993-10-13 | 1995-10-31 | Ovadia; Shmuel | System for conversion of sea wave energy |
| EP1831543A1 (en) * | 2004-12-28 | 2007-09-12 | Göran Emil Lagström | An arrangement for converting kinetic energy of ocean currents into electric energy |
| US7948106B2 (en) * | 2005-08-25 | 2011-05-24 | Institute For Energy Application Technologies Co., Ltd. | Power generator and power generation method |
| TW201014968A (en) * | 2008-10-03 | 2010-04-16 | bai-qing Liu | Direct-type wave power generation device |
| TW201016958A (en) * | 2008-10-29 | 2010-05-01 | Chun Man Cheung | A power generating device using ocean wave energy |
| KR20120120809A (en) * | 2011-04-25 | 2012-11-02 | 강성광 | aero generator |
| JP5858376B2 (en) * | 2011-06-20 | 2016-02-10 | 公立大学法人大阪市立大学 | Wave power generation system |
| CN103114959A (en) * | 2012-11-15 | 2013-05-22 | 杜志刚 | Wave corrosion resistant coast dyke shaft direct connected electricity generating device |
| CN203230521U (en) * | 2013-03-08 | 2013-10-09 | 杭州林黄丁新能源科技有限公司 | Water guiding plate device for ocean energy power generator and ocean energy power generator adopting same |
| CN203394677U (en) * | 2013-07-24 | 2014-01-15 | 宋丙钦 | Sea wave and river power generation device |
-
2015
- 2015-05-28 WO PCT/JP2015/065343 patent/WO2015190297A1/en not_active Ceased
- 2015-05-28 JP JP2016527735A patent/JPWO2015190297A1/en active Pending
- 2015-05-28 KR KR1020167037080A patent/KR20170020385A/en not_active Withdrawn
- 2015-05-28 CN CN201580012183.1A patent/CN106103977A/en active Pending
- 2015-05-29 TW TW104117301A patent/TWI638096B/en not_active IP Right Cessation
Patent Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58214678A (en) * | 1982-06-07 | 1983-12-13 | Mitsubishi Heavy Ind Ltd | Collective device of wave energy |
| US20080088132A1 (en) * | 2006-10-17 | 2008-04-17 | Laube Von Laubenfels Walter He | Wave rider |
| JP2013209978A (en) * | 2012-02-29 | 2013-10-10 | Kyb Co Ltd | Wave power generator |
Also Published As
| Publication number | Publication date |
|---|---|
| CN106103977A (en) | 2016-11-09 |
| KR20170020385A (en) | 2017-02-22 |
| JPWO2015190297A1 (en) | 2017-04-20 |
| TW201610289A (en) | 2016-03-16 |
| TWI638096B (en) | 2018-10-11 |
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