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JP2012163030A - Wind power generating device using continuity equation - Google Patents

Wind power generating device using continuity equation Download PDF

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Publication number
JP2012163030A
JP2012163030A JP2011023431A JP2011023431A JP2012163030A JP 2012163030 A JP2012163030 A JP 2012163030A JP 2011023431 A JP2011023431 A JP 2011023431A JP 2011023431 A JP2011023431 A JP 2011023431A JP 2012163030 A JP2012163030 A JP 2012163030A
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air current
cross
airflow
speed
flowout
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Takaki Shima
隆紀 島
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DATUM ISLANDS Ltd
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DATUM ISLANDS Ltd
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    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/70Wind energy
    • Y02E10/72Wind turbines with rotation axis in wind direction

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Abstract

PROBLEM TO BE SOLVED: To provide a wind power generating device which has no adverse effects on aerodynamic performance of moving bodies such as a motor vehicle, an electric train, and the like, is not affected by external contributing factors such as a flying object, rain water, and the like, and is able to control a flow rate of an air current with respect to the power generating device due to speed change of a moving object.SOLUTION: The device applies a continuity equation held for flow rates of a relative air current produced at traveling of a moving body and an air current sucked from a flowout part of the device, and guides an air current for performing wind power electricity generation into the device to generate electricity. As a structure is employed where an external air current is not directly introduced but is sucked, the air dynamic performance of a moving object is not adversely affected, and the structure is unsusceptible to external contributing factors such as a flying object, rain water, and the like. Further, flow speed at an electricity generating part can be controlled by a cross section area of the flowout part and the cross section area of the electricity generating part, and thus by providing a structure capable of controlling the cross section area of the flowout part, an arbitrary flow speed can be obtained correspondingly to the speed of the moving body, and one kind of generator can accommodate a wide range of speeds of the moving object.

Description

この発明は、自動車・電車に設置し、自動車・電車の移動により発生する気流に対する連続の方程式によって発生する気流の流れを利用した風力発電装置に関するものである。 The present invention relates to a wind turbine generator that is installed in an automobile / train and uses a flow of airflow generated by a continuous equation for an airflow generated by the movement of the automobile / train.

(イ)車両搭載発電機にプロペラを利用した風力発電装置。
(ロ)発電装置部分は車内に設置しているが、自動車・電車の前方から気流を取り入れ、発電装置を駆動させる風力発電装置。
等がある。
(B) A wind turbine generator that uses a propeller as a vehicle-mounted generator.
(B) A wind power generator that drives the power generator by taking air current from the front of the car / train, although the power generator is installed in the car.
Etc.

特許公開2003−74456Patent Publication 2003-74456 特許公開2010−31739Patent Publication 2010-31739 特許公開2003−299207Patent Publication 2003-299207

自従来の技術(イ)では、車体の外部に取り付けた部分の風を受ける面積が大きく、また発電装置が外部に露出している為、空力特性を全く無視しており、また飛来物等に対する対応も悪く、雨水に対する対応も悪い。
従来の技術(ロ)では、発電装置の駆動部分に自動車・電車の進行方向前方からの気体の流れを取り入れる為、空力特性に大きな影響を及ぼす。また、空力特性を良くする為に空気の流入口を小さくしたり、低くすると流入量が制限され、大きくすると空力特性を悪化させ、また高速運転時の流量が大きくなりすぎる場合がある。(イ)と同様に飛来物等に対する対応も悪い。
In the conventional technology (A), the area that receives the wind of the part attached to the outside of the vehicle body is large, and the power generation device is exposed to the outside, so the aerodynamic characteristics are completely ignored, and against flying objects etc. The response is bad and the response to rainwater is also bad.
In the prior art (b), since the gas flow from the front of the car / train in the traveling direction is taken into the driving part of the power generation device, the aerodynamic characteristics are greatly affected. Also, if the air inlet is made small or low to improve the aerodynamic characteristics, the inflow amount is limited, and if it is made large, the aerodynamic characteristics are deteriorated, and the flow rate at high speed operation may become too large. Like (I), the response to flying objects etc. is bad.

本装置は、図面3のように気流流入部、発電部、空洞部と気流流出部から構成される。このうち、気流流入部は、外部から直接の気流を取り入れる構造ではなく、本装置内に発生する気流を充分に供給できればどのような構造でもよい。発電部は、発電機と発電機を回転させるプロペラ部分から成る。空洞部は、発電部と気流流出部を結ぶ空洞である。気流流出部は、本装置内の気流を外部へ流出する部分であり、流出部の断面積を制御できる構造をもつ事ができる。
図面2において、自動車・電車が速度Vで走行している時に発生する相対的な気流Qを利用すると、連続の方程式により本装置の気流流出部から吸い出される気流Qbが発生する。このQbは発電部のプロペラ周囲に気流Qaを発生させ、プロペラを回転させる事ができるので、発電を行う事ができる。
気流流入部は前述のように外部から直接の気流を取り入れる構造ではないので、自動車・電車の空力性能に悪影響を及ぼすことがなく、飛来物や雨水等の外的な要因の影響を受けにくい構造とする事ができる。
また、連続の方程式から、本装置の気流流出部から吸い出される気流Qbは、発電部の気流Qaが十分であれば、自動車・電車が走行時に発生する相対的な気流Qと同じ流量となる。発電部の流速Vaは、気流流出部の気流Qb(=Q)と気流流出部の断面積と発電部のプロペラ部分の断面積により制御する事ができる。つまり、Qb(=Q)は自動車・電車の走行時の速度Vで決定され、発電部のプロペラ部分の断面積は一定と考えると、気流流出部の断面積を制御できる構造を持てば、自動車・電車の速度と制御された気流流出部の断面積により、任意のVaを得る事ができる。
これにより、低速時においては自動車・電車が走行時に発生する相対的な気流Qよりも大きなQbを得る事も可能であり、また自動車・電車が高速で運転される場合にはQより小さなQbを得る事も可能となる事を示している。また、気流流出部の面積を制御する機構を設ける事により、新幹線のような速度幅の大きな電車においても対応幅の比較的狭い発電機でも対応が可能であり、低速で走行する事が多い自動車等でも、速度によリ得られる相対的な気流より大きな流量によって発電する機構を持つ事ができる。
空気は圧縮性流体であるが、風速100メートル/秒(360キロメートル/時)位までなら動圧も低く、無視することも可能で、非圧縮性流体として扱う事が可能である。よって連続の方程式を適用する事が可能である。
As shown in FIG. 3, the present apparatus includes an airflow inflow portion, a power generation portion, a cavity portion, and an airflow outflow portion. Among these, the airflow inflow portion is not a structure that takes in a direct airflow from the outside, but may have any structure as long as the airflow generated in the apparatus can be sufficiently supplied. The power generation unit includes a generator and a propeller portion that rotates the generator. A cavity part is a cavity which connects an electric power generation part and an airflow outflow part. The airflow outflow portion is a portion through which the airflow in the apparatus flows out to the outside, and can have a structure capable of controlling the cross-sectional area of the outflow portion.
In FIG. 2, when the relative airflow Q generated when the automobile / train is traveling at the speed V is used, the airflow Qb sucked out from the airflow outflow portion of the present apparatus is generated by the continuous equation. Since this Qb can generate an air flow Qa around the propeller of the power generation unit and rotate the propeller, power generation can be performed.
As mentioned above, the airflow inflow section is not structured to take in direct airflow from the outside, so it does not adversely affect the aerodynamic performance of automobiles and trains, and is not easily affected by external factors such as flying objects and rainwater Can be.
Further, from the equation of continuity, the airflow Qb sucked out from the airflow outflow portion of the present apparatus has the same flow rate as the relative airflow Q generated when the automobile / train is running if the airflow Qa of the power generation unit is sufficient. . The flow velocity Va of the power generation section can be controlled by the airflow Qb (= Q) of the airflow outflow section, the cross-sectional area of the airflow outflow section, and the cross-sectional area of the propeller portion of the power generation section. In other words, Qb (= Q) is determined by the speed V when the car / train is running, and assuming that the cross-sectional area of the propeller part of the power generation unit is constant, if the vehicle has a structure that can control the cross-sectional area of the airflow outflow part, -Arbitrary Va can be obtained by the speed of the train and the cross-sectional area of the controlled airflow outlet.
As a result, it is possible to obtain a larger Qb than the relative air flow Q generated when the car / train is traveling at low speeds, and a smaller Qb than Q when the car / train is driven at a high speed. It shows that it can be obtained. In addition, by providing a mechanism that controls the area of the airflow outflow part, even a train with a large speed range, such as the Shinkansen, can be used with a generator with a relatively narrow range, and automobiles that often run at low speeds Etc., it is possible to have a mechanism for generating electricity with a flow rate larger than the relative airflow obtained by the speed.
Air is a compressible fluid, but if the wind speed is up to about 100 meters / second (360 kilometers / hour), the dynamic pressure is low and can be ignored, and can be treated as an incompressible fluid. Therefore, it is possible to apply a continuous equation.

(イ)進行方向前方に風の取入口等の構造を持たないので、自動車・電車の空力性能への影響を最小限に抑えることができる。
(ロ)進行方向前方に風の取入口等の構造を持たないので、飛来物や雨水等の外的な要因の影響を最小限にできる。
(ハ)気流の吸出口の大きさを変更する事により、発電装置の駆動部分の流量を制御できるので、自動車・電車の速度の変化に対して最大限の効率で発電する事ができる。
(二)新幹線のような速度幅の大きな電車においても対応幅の比較的狭い発電機でも対応が可能である。
(ホ)自動車・電車の走行により車体の周りに発生する気流を利用するので、天候に左右されない発電量を確保できる。特に電車の場合は運行ダイアに従い、計画的な発電量を確保できる。
(A) Since there is no structure such as a wind inlet in the forward direction, the influence on the aerodynamic performance of automobiles and trains can be minimized.
(B) Since there is no structure such as a wind intake in front of the traveling direction, the influence of external factors such as flying objects and rainwater can be minimized.
(C) By changing the size of the airflow suction port, the flow rate of the drive part of the power generation device can be controlled, so that it is possible to generate power with maximum efficiency against changes in the speed of automobiles and trains.
(2) Even a train with a large speed range such as the Shinkansen can be used with a generator with a relatively narrow range.
(E) Since the airflow generated around the vehicle body by driving a car or train is used, it is possible to secure a power generation amount that is not affected by the weather. In particular, in the case of trains, the planned power generation can be secured according to the operation diagram.

連続の方程式においては、a点とb点での流量は同じである。ここに、a点での流速をVaとし、b点での流速をVbとすると、VaとVbの間にはa点の面積とb点の面積比に対し、反比例の関係になる。よって、b点での流量を一定とした場合、a点の流速はb点の面積により制御する事ができる。流体を空気で考えた場合、前述のように空気は圧縮性流体であるが、一定の流速以下では非圧縮性流体として扱う事が可能である事から、本発明を電車・自動車等に応用する事が可能である。In the continuity equation, the flow rates at points a and b are the same. If the flow velocity at point a is Va and the flow velocity at point b is Vb, the relationship between Va and Vb is inversely proportional to the area ratio of point a and the area of point b. Therefore, when the flow rate at point b is constant, the flow velocity at point a can be controlled by the area at point b. When the fluid is considered to be air, as described above, air is a compressible fluid, but it can be handled as an incompressible fluid below a certain flow rate, and therefore the present invention is applied to trains, automobiles, etc. Things are possible. 電車や自動車が走行時に発生する相対的な気流の流量をQとした場合、A点に設置した発電装置の流入口側に充分な流量Qaがある場合、流出口B点の流量Qbは外部の流量Qと同じとなる。従って、A点に設置した発電装置を駆動する流量QaはB点の流出口の面積とAに設置した発電装置の断面積により、外部の流量Qに対して面積比で算出でき、また制御する事ができる。本装置では、A点の流量Qaを確保する必要があるが、電車や自動車の走行時にそれらの空力性能に悪影響を及ぼすことなく、飛来物や雨水等の外的な要因の影響を受けないような形状とする必要がある。Assuming that the flow rate of the relative air flow generated when the train or car is running is Q, if there is a sufficient flow rate Qa on the inlet side of the power generator installed at the point A, the flow rate Qb at the outlet B point is external. It becomes the same as the flow rate Q. Therefore, the flow rate Qa for driving the power generator installed at the point A can be calculated and controlled by the area ratio with respect to the external flow rate Q based on the area of the outlet at the point B and the cross-sectional area of the power generator installed at the point A. I can do things. In this device, it is necessary to secure the flow rate Qa at point A, but it does not adversely affect the aerodynamic performance of trains and cars, and is not affected by external factors such as flying objects and rainwater. It is necessary to make it a simple shape. 図面2において、A点に設置した発電装置の断面積は一定であり、Qaを制御する為にはB点の流出口の面積を制御すればよい事になる。実際の適用例としては、C部に発電装置を設置し、D部に発電装置を駆動する為のプロペラ等の装置を設置する。流出口となるE部には、例えばフラッパ機能等を設置して面積を制御できるようにする。In FIG. 2, the cross-sectional area of the power generator installed at the point A is constant, and the area of the outlet at the point B may be controlled in order to control the Qa. As an actual application example, a power generation device is installed in the C section, and a device such as a propeller for driving the power generation apparatus is installed in the D section. For example, a flapper function or the like is installed in the E portion serving as the outflow port so that the area can be controlled. 電車においては、図面3で示した発電装置を複数個、それぞれの流出口からの気流の影響を受けないような縦/横方向への配置をする事により、一車両に複数個を設置する事も可能である。ただし、電車に於いては両方向に進行する事に対する配置上の配慮が必要となる。In a train, a plurality of power generators shown in FIG. 3 are arranged in a vertical / horizontal direction so as not to be affected by the airflow from the respective outlets. Is also possible. However, on a train, it is necessary to consider the arrangement for traveling in both directions. 自動車においては、図面3で示した発電装置を進行方向に平行に複数個配置をする事により、一車両に数個を設置する事も可能である。また、バスや運搬車両の場合は、上記電車の場合のような配置が可能であり、また進行方向の配慮も要らないので大きなエネルギーを得る事が可能となる。In an automobile, it is possible to install several power generators shown in FIG. 3 in one vehicle by arranging a plurality of power generators parallel to the traveling direction. In the case of a bus or a transport vehicle, it can be arranged as in the case of the above-mentioned train, and it is not necessary to consider the direction of travel, so that a large amount of energy can be obtained. 電気自動車等に適応する場合は、従来の自動車に比べエンジン部に比べ余裕が考えられるので、フロント部分に本装置を配置する事により、車高を変更せず、また室内空間を圧迫する事なく設置する事が可能である。When adapting to electric vehicles, etc., there is a margin compared to the engine part compared to conventional cars, so placing this device in the front part does not change the vehicle height and does not compress the indoor space It is possible to install.

(イ)電車の屋外に設置し、計画的な発電を行い、走行用/空調用等の電気エネルギーとして利用する
(ロ)電気自動車・ハイブリッド自動車に設置し、電気エネルギーとして利用する
(ハ)保冷車に設置し、保冷用電気エネルギーとして利用する
(二)一般車両の電気エネルギー(エアコン用途他)として
(ホ)走行時にバッテリー等に蓄電し、売却(ガソリンスタンドや自宅から)
(B) Installed outdoors on trains for planned power generation and used as electric energy for driving / air conditioning, etc. (b) Installed in electric vehicles / hybrid vehicles and used as electric energy (c) Cold storage Installed in a car and used as electric energy for cold storage (2) Stored in a battery, etc., when sold (from a gas station or home)

なし None

現在、風力発電用の小型発電機の開発も進展しており、電車や大型の自動車/バス等においてはすぐにでも利用可能な技術である。また、小型/中型自動車においても本装置の配置方法の工夫や更なる小型発電機の開発により十分利用可能な技術である。自動車/バスにおいては、それ自身が電気動力でない場合で発電したエネルギーを蓄電する必要がある場合も、電気自動車の実用化が進む現在ではバッテリー技術も向上しており、対応に問題は無い。その蓄電した電気を自宅等において電力会社に販売する装置等も家屋屋上での太陽光発電等による技術を応用すれば問題ないはずである。 Currently, the development of small generators for wind power generation is also progressing, and it is a technology that can be used immediately in trains, large cars / buses, and the like. In addition, this technology can be used sufficiently even in small / medium-sized automobiles by devising the arrangement method of this apparatus and developing a further small generator. In the automobile / bus, even when it is necessary to store the generated energy when it is not electric power itself, the battery technology is improved at present when the electric vehicle is put into practical use, and there is no problem in dealing with it. Devices that sell the stored electricity to an electric power company at home or the like should have no problem if a technique such as solar power generation on the roof of the house is applied.

図1 a :任意の断面位置a
図1 Va:任意の断面位置aの流速
図1 b :任意の断面位置b
図1 Vb:任意の断面位置bの流速
図2 Q :電車や自動車が走行時、回りに発生する相対的な気流の流量
図2 A :発電装置を設置している位置
図2 Qa:A点に設置した発電装置付近の流量
図2 B :発電装置からの流出口
図2 Qb:B点の流量
図2 V :電車や自動車の走行速度
図3 C :発電装置
図3 D :発電装置を駆動する為のプロペラ等の装置
図3 E :流出口
FIG. 1 a: Arbitrary sectional position a
Fig. 1 Va: Flow velocity at an arbitrary cross-sectional position a 1 b: Arbitrary cross-sectional position b
Fig. 1 Vb: Flow velocity at an arbitrary cross-sectional position b 2 Q: Flow rate of relative airflow generated around a train or automobile traveling 2 A: Location where a power generator is installed 2 Qa: Point A Fig. 2 Flow rate near the power generator installed in Fig. 2 B: Outlet from the power generator Fig. 2 Qb: Flow rate at point B 2 V: Traveling speed of trains and cars 3C: Power generator Fig. 3 D: Drive the power generator Fig. 3 E: Outlet

Claims (2)

自動車・電車に設置して走行時に連続の方程式に従い発生する気流を利用した風力発電装置 A wind turbine generator that uses airflow generated according to a continuous equation when running on an automobile or train 請求項1において、吸出口の面積を制御する事により発電装置の気流の速さを調節できるようにするための装置を有する風力発電装置 2. The wind turbine generator according to claim 1, further comprising a device for controlling the airflow speed of the power generator by controlling the area of the suction port.
JP2011023431A 2011-02-06 2011-02-06 Wind power generating device using continuity equation Withdrawn JP2012163030A (en)

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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107882685A (en) * 2017-11-20 2018-04-06 刘大康 A kind of wind generator system positioned at subway carriage afterbody
CN108656961A (en) * 2018-05-09 2018-10-16 罗远林 It is a kind of to utilize the hydroelectric new-energy automobile of wind-force rain

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107882685A (en) * 2017-11-20 2018-04-06 刘大康 A kind of wind generator system positioned at subway carriage afterbody
CN108656961A (en) * 2018-05-09 2018-10-16 罗远林 It is a kind of to utilize the hydroelectric new-energy automobile of wind-force rain

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