JPS621106B2 - - Google Patents
Info
- Publication number
- JPS621106B2 JPS621106B2 JP55143865A JP14386580A JPS621106B2 JP S621106 B2 JPS621106 B2 JP S621106B2 JP 55143865 A JP55143865 A JP 55143865A JP 14386580 A JP14386580 A JP 14386580A JP S621106 B2 JPS621106 B2 JP S621106B2
- Authority
- JP
- Japan
- Prior art keywords
- eccentric rotating
- floating body
- rotating body
- energy
- rotation
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 230000033001 locomotion Effects 0.000 claims description 19
- 238000000034 method Methods 0.000 claims description 18
- 238000006243 chemical reaction Methods 0.000 claims description 10
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 claims description 9
- 230000005540 biological transmission Effects 0.000 claims description 6
- 230000005284 excitation Effects 0.000 description 7
- 230000005484 gravity Effects 0.000 description 6
- 230000010355 oscillation Effects 0.000 description 5
- 230000001133 acceleration Effects 0.000 description 2
- 230000003247 decreasing effect Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 239000000284 extract Substances 0.000 description 2
- 238000010248 power generation Methods 0.000 description 2
- 238000005260 corrosion Methods 0.000 description 1
- 230000007797 corrosion Effects 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000001902 propagating effect Effects 0.000 description 1
- 230000001360 synchronised effect Effects 0.000 description 1
Classifications
-
- 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
Landscapes
- Other Liquid Machine Or Engine Such As Wave Power Use (AREA)
Description
【発明の詳細な説明】
本発明は波浪エネルギーの変換方法に関する。
更に詳しくは、偏心回転体の回転周期と、該回転
体を塔載し波浪により揺動する浮体の揺動周期と
を共振もしくは共振に近い状態に保つことによ
り、波浪エネルギーを効率良く偏心回転体の運動
エネルギーに変換する方法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for converting wave energy.
More specifically, by keeping the rotation period of the eccentric rotating body and the oscillation period of the floating body on which the rotating body is mounted, which is rocked by the waves, in a state of resonance or close to resonance, wave energy can be efficiently transferred to the eccentric rotating body. Concerning how to convert into kinetic energy.
波浪エネルギーを電力に転換する波浪発電のた
めのエネルギー変換方法には種々のタイプのもの
が知られている。例えば波力により浮体が上下動
する際に生じる該浮体と周囲の水との速度差によ
り浮体下部に取付られたプロペラが回転し、発電
機を駆動する波浪発電機関において、波のエネル
ギーの変換効率を高めるため、該浮体と波の上下
動周期を同調させる方法が開示されている(特開
昭51−86639)。しかしこの方法には、上記の上下
動周期の調整のための浮力調節装置の他に、波の
周期毎に起る順逆両方向の水流よりスムーズな一
方向の回転を取り出す装置、さらに水中に露出し
た可動部の腐食や水生生物の付着による効率低下
への対策など問題点が多い。 Various types of energy conversion methods are known for converting wave energy into electric power for wave power generation. For example, when a floating body moves up and down due to wave force, the speed difference between the floating body and the surrounding water causes a propeller attached to the bottom of the floating body to rotate, and in a wave power generation engine that drives a generator, the conversion efficiency of wave energy is In order to increase this, a method has been disclosed in which the vertical motion period of the floating body and waves are synchronized (Japanese Patent Laid-Open No. 51-86639). However, this method requires, in addition to the above-mentioned buoyancy adjustment device for adjusting the vertical movement period, a device that extracts smoother rotation in one direction than the forward and reverse water flow that occurs every wave period, and a There are many problems, such as countermeasures to reduce efficiency due to corrosion of moving parts and adhesion of aquatic organisms.
本発明者は上記の諸問題を解決すべく鋭意研究
の結果波浪による浮体の揺動を該浮体の内部に設
置された発生機内の偏心回転体の回転運動エネル
ギーに変換することにより、前述の問題点が解決
できることを知り本発明に到つたものである。す
なわち本発明の目的は、浮体を用いた波浪エネル
ギー変換方法において、該浮体の浮力調節装置及
び水中に可動部を持たず、且波浪の運動よりスム
ーズな一方向の回転に係る回転エネルギーを取り
出すことのできる波浪エネルギー変換方法の提供
にある。 As a result of intensive research in order to solve the above-mentioned problems, the present inventor has solved the above-mentioned problems by converting the rocking motion of a floating body caused by waves into rotational kinetic energy of an eccentric rotating body in a generator installed inside the floating body. The present invention was developed based on the knowledge that this problem could be solved. That is, an object of the present invention is to provide a wave energy conversion method using a floating body, which does not have a buoyancy adjustment device or a moving part in the water, and extracts rotational energy related to rotation in one direction that is smoother than wave motion. The purpose of the present invention is to provide a wave energy conversion method that allows for
本発明は、下記第(1)及び第(2)項の波浪エネルギ
ー変換方法である。 The present invention is a method for converting wave energy according to the following items (1) and (2).
(1) 水面もしくは水中に設置せられ波浪により揺
動する浮体とその内部に取付けられた偏心回転
体を有する発生機および該発生機内の該偏心回
転体と回転軸を通じて接続された変速機構から
なる装置を用い、該装置から外部に取り出すエ
ネルギーを調整することにより該偏心回転体の
回転周期を該浮体の揺動周期と共振もしくは共
振に近い状態に保つことを特徴とする該浮体の
受ける波浪エネルギーを偏心回転体の回転運動
エネルギーに変換する波浪エネルギー変換方
法。(1) Consisting of a floating body installed on the water surface or in the water that is rocked by waves, a generator having an eccentric rotating body installed inside the floating body, and a transmission mechanism connected to the eccentric rotating body in the generator through a rotating shaft. Wave energy received by the floating body, characterized in that the rotation period of the eccentric rotating body is kept at resonance or close to resonance with the oscillation period of the floating body by using a device and adjusting the energy taken out from the device to the outside. A method of converting wave energy into rotational kinetic energy of an eccentric rotating body.
(2) 対をなす偏心回転体を互に反対方向に回転さ
せ、該回転に任意且一定の位相差をもたせるこ
とにより、浮体の揺動エネルギーの水平方向成
分および垂直方向成分を該位相差に応じた割合
で該偏心回転体の回転運動エネルギーに変換す
る上記第(1)項の波浪エネルギー変換方法。(2) By rotating a pair of eccentric rotating bodies in opposite directions and creating an arbitrary and constant phase difference in the rotation, the horizontal and vertical components of the rocking energy of the floating body are adjusted to the phase difference. The wave energy conversion method according to item (1) above, wherein the wave energy conversion method converts into rotational kinetic energy of the eccentric rotating body at a proportion according to the ratio.
以下に本発明の構成と効果を図面によつて詳細
に説明する。第1図は本発明に係る偏心回転体の
回転軸に直角な方向の断面説明図である。同図に
おいて、偏心回転体の重量をW、回転軸Oより重
心Dまでの距離をdとし、偏心回転体がOを中心
とし一様な角速度pで回転する場合、遠心力に相
当する力、F=(W/g)p2d、が軸受を経て起
振力として作用する(gは重力の加速度)。回転
軸に垂直な互に直交する二方向をX、Yとする
と、前記起振力のY方向成分は、
Fy=(W/g)p2d cos pt (1)
で表わされる(註.時間t=Oのとき、重心がY
軸上にあり、逆時計方向に回転するものとす
る)。 The configuration and effects of the present invention will be explained in detail below with reference to the drawings. FIG. 1 is an explanatory cross-sectional view of the eccentric rotating body according to the present invention in a direction perpendicular to the rotation axis. In the figure, the weight of the eccentric rotating body is W, the distance from the rotation axis O to the center of gravity D is d, and when the eccentric rotating body rotates around O at a uniform angular velocity p, a force equivalent to centrifugal force, F=(W/g)p 2 d acts as an excitation force via the bearing (g is the acceleration of gravity). Assuming that the two mutually orthogonal directions perpendicular to the axis of rotation are X and Y, the Y-direction component of the excitation force is expressed as Fy=(W/g)p 2 d cos pt (1) (Note: Time When t=O, the center of gravity is Y
on the shaft and rotating counterclockwise).
今、偏心回転体を含む系全体が、回転軸Oを中
心とし、振幅2AのY軸に平行な往複運動を行な
うものとし、その移動量yが
y=Asin(ωt+α) (2)
で表されるものとする(ただしωは単振動の角振
動数、αはその初位相を示す)。ここで、偏心回
転体の回転と上記往復運動とが共振する場合に
は、p=ω、α=Oとなり、この往復運動より偏
心回転体が受取るエネルギーUは、以下のように
算出される。 Now, the entire system including the eccentric rotating body is assumed to perform reciprocating motion parallel to the Y-axis with an amplitude of 2A centered around the rotation axis O, and the amount of movement y is expressed as y=Asin(ωt+α) (2) (where ω is the angular frequency of simple harmonic vibration and α is its initial phase). Here, when the rotation of the eccentric rotor and the reciprocating motion resonate, p=ω and α=O, and the energy U received by the eccentric rotor from this reciprocating motion is calculated as follows.
偏心回転体を含む系が共振状態において微小距
離dyだけ移動する間になされる仕事dUは、
dU=F・dy=(W/g)dp2・cospt・dy (3)
一方、dy=(dy/dt)・dt、dy/dt=Ap・cospt
であるから、
dU=(W/g)dp3A・cos2pt・dt (4)
従つて半周期間になされる仕事U′は
U′=∫A −AF・dy=∫〓/P D(W/g)dp3A・cos2pt・dt=(W/g)dp3A〔(t/2)
+(1/4p)・sin2pt〕〓/p D=(W/2g)dp2Aπ
単位時間当りになされる仕事Uは
U=(W/2g)dp3A (5)
で表わされ、これは偏心回転体が共振状態で受取
るエネルギーに等しい。 The work dU done while the system including the eccentric rotating body moves by a minute distance dy in a resonant state is dU=F・dy=(W/g)dp 2・cospt・dy (3) On the other hand, dy=(dy /dt)・dt, dy/dt=Ap・cospt
Therefore, dU=(W/g)dp 3 A・cos 2 pt・dt (4) Therefore, the work U′ done during a half period is U′=∫ A −A F・dy=∫〓 /P D (W/g)dp 3 A・cos 2 pt・dt=(W/g)dp 3 A [(t/2) + (1/4p)・sin2pt]〓 /p D = (W/2g)dp 2 Aπ The work done per unit time U is expressed as U=(W/2g)dp 3 A (5), which is equal to the energy received by the eccentric rotating body in a resonant state.
さて深さが波長の1/2以上の深海を伝搬する波
の運動は正弦波に近似されるので、その深海に浮
び浮体の上下運動もほぼ正弦波の単振動と考えて
よい。偏心回転体の回転が、これを載せた浮体の
上下運動を共振する状態に制御されれば、該回転
体は上記(5)式に相当するエネルギーを受取ること
になり、このエネルギーを回転体の回転軸より定
常的に取り出すことができる。この場合共振状態
から外れる度合に応じて偏心回転体の受取るエネ
ルギーが減少する。このようなエネルギーの変換
率の低下を許容すれば、厳密な意味での共振状態
の実現、保持は必ずしも必要ではなく、共振に近
い状態に保たれれば実用上差支えない。 Now, since the motion of waves propagating in the deep ocean, where the depth is more than 1/2 of the wavelength, is approximated to a sine wave, the vertical motion of a floating body in the deep ocean can also be considered to be a simple harmonic motion of a sine wave. If the rotation of the eccentric rotating body is controlled so that it resonates with the vertical motion of the floating body on which it is mounted, the rotating body will receive energy corresponding to equation (5) above, and this energy will be transferred to the rotating body. It can be taken out regularly from the rotating shaft. In this case, the energy received by the eccentric rotating body decreases depending on the degree to which it deviates from the resonance state. If such a reduction in the energy conversion rate is allowed, it is not necessarily necessary to achieve or maintain a resonant state in the strict sense, and there is no practical problem as long as a state close to resonance is maintained.
本発明を以下に述べる実施態様例によつて更に
説明する。第2図は本発明に係る波浪エネルギー
変換装置を塔載した浮体Eの横断面図、第3図は
同じく縦断面図である。第2図において、一対の
偏心回転体G,G′は浮体Eの長軸方向の中心線
に対称に設置され、回転軸H,H′は浮体Eの長
軸方向に平行且水平に位置する。偏心回転体G,
G′が浮体Eの中心線に対し対称な位置を保ちな
がら互に逆方向に等速度回転する場合の起振力
F′は、式(1)より
F′=2(W/g)dp2・cospt
であり、その作用点は2つの軸H,H′の中央
で、力の方向はHH′の作る平面に垂直である。 The invention will be further illustrated by the following embodiment examples. FIG. 2 is a cross-sectional view of a floating body E on which a wave energy conversion device according to the present invention is mounted, and FIG. 3 is a longitudinal cross-sectional view thereof. In Fig. 2, a pair of eccentric rotating bodies G and G' are installed symmetrically about the center line in the long axis direction of the floating body E, and the rotation axes H and H' are located parallel and horizontal to the long axis direction of the floating body E. . Eccentric rotating body G,
Excitation force when G' rotates at a constant speed in opposite directions while maintaining a symmetrical position with respect to the center line of floating body E
From equation (1), F' is F'=2(W/g)dp 2・cospt, and its point of action is at the center of the two axes H and H', and the direction of the force is on the plane created by HH'. Vertical.
浮体Eの上下運動が式(2)で表わされ、この運動
と重量がそれぞれWである偏心回転体G,G′の
運動が共振した場合、該偏心回転体G,G′が単
位時間当りに受取るエネルギーは、式(3)、(4)およ
び(5)と同様にして、
U=(W/g)dAp3
で与えられる。今、偏心回転体G,G′の重量
(W)が回転軸の長さ当りそれぞれ63T/m、d
=3.2mで浮体Eの運動がA=2.5m、p=
0.785rad(周期約8秒)とすると、回転軸H,
H′の方向1m当り24KWのエネルギーが取出せる
ことになる。 The vertical motion of the floating body E is expressed by equation (2), and if this motion resonates with the motion of the eccentric rotating bodies G, G' whose weights are W, then the eccentric rotating bodies G, G' per unit time The energy received by is given by U=(W/g)dAp 3 , similar to equations (3), (4) and (5). Now, the weights (W) of the eccentric rotating bodies G and G' are 63T/m and d, respectively, per the length of the rotating shaft.
= 3.2m, the motion of floating body E is A = 2.5m, p =
If it is 0.785rad (period approximately 8 seconds), the rotation axis H,
This means that 24KW of energy can be extracted per meter in the direction of H'.
第3図において、起動電動機Lによりあらかじ
め浮体Eの揺動周期と共振に近い回転周期に偏心
回転体G,G′を起動する。浮体Eの上下動によ
り偏心回転体G,G′に与えられたエネルギー
は、回転軸H,H′より増速機Mを介し発電機N
に伝えられ、交流電力に変換された後、交直変換
機Qにより直流電力に変換され、ケーブルRを通
して送出される。交直変換機Qの直流出力を制御
することにより、発電機Nの負荷を増減させ、ひ
いては偏心回転体G,G′の回転周期が制御され
る。 In FIG. 3, the eccentric rotating bodies G and G' are started in advance by a starting motor L at a rotation period close to the oscillation period of the floating body E and resonance. The energy given to the eccentric rotating bodies G, G' by the vertical movement of the floating body E is transferred from the rotating shafts H, H' to the generator N via the speed increaser M.
After being converted to AC power, the AC power is converted to DC power by an AC/DC converter Q, and then sent out through a cable R. By controlling the DC output of the AC/DC converter Q, the load on the generator N is increased or decreased, and the rotation periods of the eccentric rotors G and G' are thereby controlled.
すなわち交直変換機の出力は、浮体の揺動の振
幅、周期、位相ならびに偏心回転体の回転周期お
よび位相を検出し、偏心回転体の回転周期が浮体
の揺動周期に対し速くなる傾向にあれば前記変換
機の出力を増し、逆に遅くなる傾向にあれば出力
を減らすように(場合によつては外部からエネル
ギーを加えて)制御される。このようにすれば非
線系自励振系における周期数引き込み現象により
偏心回転体の回転周期は常に浮体の揺動周期と共
振もしくは共振に近い状態に保たれる。 In other words, the output of the AC/DC converter detects the amplitude, period, and phase of the oscillation of the floating body as well as the rotation period and phase of the eccentric rotating body, and detects whether the rotation period of the eccentric rotating body tends to be faster than the oscillating period of the floating body. If the converter tends to become slower, the output is increased, and if the converter tends to become slower, the output is decreased (in some cases by applying external energy). In this way, the rotation period of the eccentric rotating body is always maintained at or near resonance with the oscillation period of the floating body due to the period number pull-in phenomenon in the nonlinear self-excited system.
偏心回転体の回転周期および位相は、例えば回
転軸H,H′に回転計を設けることにより検出す
る。浮体の揺動の振幅、周期および位相は、例え
ば○イ該浮体に設置された位置計、速度計、加速度
計、水位計、水圧計等の測定値から求め、○ロある
いは上記○イで求められた値を時間軸に対し外挿す
ることにより予測し、もしくは○ハ該浮体とは別に
設けられた波浪計等により検出される波浪の周期
および波高等の値より算出する。○イの方法によれ
ば、前記出力制御はフイードバツク方式となり、
○ロ、○ハの方法によればフイードフオワード方式を
とることが可能である。 The rotation period and phase of the eccentric rotating body are detected, for example, by providing tachometers on the rotating shafts H and H'. The amplitude, period, and phase of the rocking of a floating body can be determined, for example, from the measured values of the position meter, speedometer, accelerometer, water level gauge, water pressure gauge, etc. installed on the floating body in ○a, and determined in ○b or ○a above. It is predicted by extrapolating the determined value to the time axis, or it is calculated from the wave period and wave height values detected by a wave meter etc. installed separately from the floating body. According to method ○a, the output control is a feedback method,
According to methods ○B and ○C, it is possible to adopt a feed-forward method.
以下に本発明の実施態様例のいくつかを示す。 Some embodiments of the present invention are shown below.
(a) 第3図において、交直変換機Qを設けず、増
速機Mと交流発電機Nとの間に無段変速機を設
置し、該発電機は一定回転数で運動せられ、偏
心回転体の速度制御は上記無段変速機を介して
行なう方法。(a) In Fig. 3, an AC/DC converter Q is not provided, but a continuously variable transmission is installed between a speed increaser M and an AC generator N, and the generator is operated at a constant rotation speed and eccentrically In this method, the speed of the rotating body is controlled via the above-mentioned continuously variable transmission.
(b) 第3図において、交直変換機Qを設けず、発
電機Nを直流発電機とし、偏心回転体の速度制
御は該直流発電機の出力制御で行う方法。(b) In Fig. 3, a method in which the AC/DC converter Q is not provided, the generator N is a DC generator, and the speed of the eccentric rotating body is controlled by the output control of the DC generator.
(c) 第3図において、発電機N、交直変換機Q、
ケーブルRをいずれも設けず、発生機Kの出力
を増速機Mおよび無段変速機を経てフライホイ
ール等の適当な機械系に導き、運動のエネルギ
ーとして取出し、該偏心回転体の速度並びに出
力の制御は該無段変速機を介して行なう方法。(c) In Figure 3, generator N, AC/DC converter Q,
Without providing any cable R, the output of the generator K is guided to a suitable mechanical system such as a flywheel via a speed increaser M and a continuously variable transmission, and is extracted as kinetic energy, thereby increasing the speed and output of the eccentric rotating body. control is performed via the continuously variable transmission.
(d) 偏心回転体G,G′の回転に任意且一定の位
相差をもたせ、起振力に水平方向の分力を持た
せることにより、浮体Eの水平方向の移動エネ
ルギーをも併せて吸収させる方法(第4図参
照)。(d) By giving an arbitrary and constant phase difference to the rotation of the eccentric rotating bodies G and G' and giving a horizontal component to the excitation force, the horizontal movement energy of the floating body E is also absorbed. (See Figure 4).
第1図は偏心回転体の回転と起振力の説明図、
第2図は波浪エネルギー変換装置を塔載した浮体
の横断面図、第3図は該浮体の縦断面図、第4図
は偏心回転体の位相と起振力の方向の説明図であ
る。これらの図面において各記号は、W;偏心回
転体の重量、D;偏心回転体の重心、O;回転
軸、d;重心と回転軸の距離、p;角速度、g;
重力の加速度、E;浮体、GおよびG′;偏心回
転体、HおよびH′;回転軸、K;発生機、L;
起動用電動機、N;発電機、Q;交直変換機、
R;ケーブル、S;起振力の方向を表す。
Figure 1 is an explanatory diagram of the rotation of the eccentric rotating body and the excitation force.
FIG. 2 is a cross-sectional view of a floating body on which a wave energy conversion device is mounted, FIG. 3 is a vertical cross-sectional view of the floating body, and FIG. 4 is an explanatory diagram of the phase of the eccentric rotating body and the direction of the excitation force. In these drawings, each symbol is W: weight of the eccentric rotating body, D: center of gravity of the eccentric rotating body, O: axis of rotation, d: distance between the center of gravity and the axis of rotation, p: angular velocity, g;
Acceleration of gravity, E; Floating body, G and G'; Eccentric rotating body, H and H'; Axis of rotation, K; Generator, L;
Starting motor, N: generator, Q: AC/DC converter,
R: cable, S: direction of excitation force.
Claims (1)
動する浮体と該浮体内部に取付けられた偏心回転
体を有する発生機および該発生機内の該偏心回転
体と回転軸を通じて接続された変速機構からなる
装置を用い、該装置から外部へ取り出すエネルギ
ーを調整することにより該偏心回転体の回転を該
浮体の揺動と共振もしくは共振に近い状態に保つ
ことを特徴とする該浮体の受ける波浪エネルギー
を偏心回転体の回転運動エネルギーに変換する波
浪エネルギー変換方法。 2 対をなす偏心回転体を互に反対方向に回転さ
せ、該回転に任意且一定の位相差をもたせること
により、浮体の揺動エネルギーの水平方向成分お
よび垂直方向成分を該位相差に応じた割合で該偏
心回転体の回転運動エネルギーに変換する特許請
求の範囲第1項記載の波浪エネルギー変換方法。[Claims] 1. A generator having a floating body disposed on the water surface or in the water and rocked by waves, an eccentric rotating body installed inside the floating body, and a generator connected to the eccentric rotating body in the generator through a rotating shaft. The floating body is characterized in that the rotation of the eccentric rotating body is maintained at or near resonance with the rocking motion of the floating body by using a device consisting of a transmission mechanism and adjusting the energy taken out from the device to the outside. A wave energy conversion method that converts received wave energy into rotational kinetic energy of an eccentric rotating body. 2. By rotating a pair of eccentric rotating bodies in opposite directions and giving an arbitrary and constant phase difference to the rotation, the horizontal and vertical components of the rocking energy of the floating body can be adjusted according to the phase difference. 2. The method of converting wave energy according to claim 1, wherein the wave energy is converted into rotational kinetic energy of the eccentric rotating body at a ratio of 1 to 3.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP55143865A JPS5768566A (en) | 1980-10-15 | 1980-10-15 | Converting method of waste energy |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP55143865A JPS5768566A (en) | 1980-10-15 | 1980-10-15 | Converting method of waste energy |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5768566A JPS5768566A (en) | 1982-04-26 |
JPS621106B2 true JPS621106B2 (en) | 1987-01-12 |
Family
ID=15348779
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP55143865A Granted JPS5768566A (en) | 1980-10-15 | 1980-10-15 | Converting method of waste energy |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5768566A (en) |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5343146B2 (en) * | 1973-03-14 | 1978-11-17 |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5343146U (en) * | 1976-09-17 | 1978-04-13 |
-
1980
- 1980-10-15 JP JP55143865A patent/JPS5768566A/en active Granted
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5343146B2 (en) * | 1973-03-14 | 1978-11-17 |
Also Published As
Publication number | Publication date |
---|---|
JPS5768566A (en) | 1982-04-26 |
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