JPH0310118A - Flow-rate detecting apparatus - Google Patents

Flow-rate detecting apparatus

Info

Publication number
JPH0310118A
JPH0310118A JP14593889A JP14593889A JPH0310118A JP H0310118 A JPH0310118 A JP H0310118A JP 14593889 A JP14593889 A JP 14593889A JP 14593889 A JP14593889 A JP 14593889A JP H0310118 A JPH0310118 A JP H0310118A
Authority
JP
Japan
Prior art keywords
magnetic
permanent magnet
flow
flow rate
swirling
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.)
Granted
Application number
JP14593889A
Other languages
Japanese (ja)
Other versions
JPH0765912B2 (en
Inventor
Yukinori Ozaki
行則 尾崎
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP14593889A priority Critical patent/JPH0765912B2/en
Publication of JPH0310118A publication Critical patent/JPH0310118A/en
Publication of JPH0765912B2 publication Critical patent/JPH0765912B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PURPOSE:To make it possible to detect a low flow rate by rotating a magnetic spherical body at the low flow rate even under the state wherein the magnetic spherical body is attracted to the side of a permanent magnet. CONSTITUTION:When a detecting apparatus is filled with a fluid, a magnetic spherical body 27 whose specific gravity is close to 1 is attracted to the side of a permanent magnet 35 with the magnetic force of the permanent magnet 35. When the fluid to be detected flows in the direction of an arrow under this state, the fluid to be detected is jetted through jetting ports 30 - 32 of a fixed blade 25, and a swirling stream is formed. Thus, the spherical body 27 is turned. At this time, an angle alpha between a hub 24 and a blade 23 is made larger than an angles alpha between other blades 21 and 22 and the hub 24. Therefore, the areas of the jetting ports 31 and 32 are made smaller than the area of the jetting port 30. Thus, the flow speed at the jetting port 31 through which the swirling stream that collides the stationary spherical body 27 at a position facing the permanent magnet 27 becomes faster than the flow speed of the stream jetted through the other jetting port 30. Since the collision energy to the spherical body 27 becomes large, the spherical body 27 starts turning at the low flow rate. Therefore, even if the magnetic spherical body is attracted to the permanent magnet, the low flow rate can be detected.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は給湯装置や温水暖房装置の水又は湯の流量を検
出したり、液体燃料供給装置の燃料流量を検出する目的
で使用する流体検出装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a fluid detection device used for the purpose of detecting the flow rate of water or hot water in a water heater or hot water heating device, or for detecting the fuel flow rate in a liquid fuel supply device. It is something.

従来の技術 従来この種の流量検出装置としては第3図、第4図に示
すようなものがある。第3図、第4図で1はハウジング
である。このハウジング1の内部には流体を旋回流とす
るための複数の翼2、翼3、翼4で構成される固定翼5
が流路内壁6に密着して設けられている。前記固定翼5
の下流には流路内をrfJ回する磁性球体7が設けられ
ている。この磁性球体7は内部に磁性金属中空球を有し
外部を樹脂モールドし、水中等においての比重はほぼ1
.0に近い構成である。この磁性球体7の下流には前記
磁性球体7が下流側へ流出するのを防止すると共に前記
磁性球体7の周回当接面8を有する球体受け9が設けら
れている。又ハウジング1の外部には、前記磁性球体7
の回転を検出する検出器10が設けられている。この検
出器10は磁気抵抗素子11とこの磁気抵抗素子11に
磁界を与える永久磁石12と前記磁気抵抗素子11の出
力信号を処理する電子回路13が設けられている。14
.15.16は旋回流の流れ方向を示す流線であり、1
7.18.19は各々旋回流を噴出する噴出口である。
2. Description of the Related Art Conventionally, this type of flow rate detection device is shown in FIGS. 3 and 4. In FIGS. 3 and 4, 1 is a housing. Inside this housing 1 is a fixed wing 5 which is composed of a plurality of wings 2, 3, and 4 for making the fluid into a swirling flow.
is provided in close contact with the inner wall 6 of the flow path. Said fixed wing 5
A magnetic sphere 7 that rotates rfJ in the flow path is provided downstream of the flow path. This magnetic sphere 7 has a magnetic metal hollow sphere inside, the outside is molded with resin, and its specific gravity in water etc. is approximately 1.
.. This is a configuration close to 0. A sphere receiver 9 is provided downstream of the magnetic sphere 7, which prevents the magnetic sphere 7 from flowing out to the downstream side and has a rotating contact surface 8 for the magnetic sphere 7. Further, the magnetic sphere 7 is provided on the outside of the housing 1.
A detector 10 is provided to detect the rotation of. This detector 10 is provided with a magnetoresistive element 11, a permanent magnet 12 that applies a magnetic field to the magnetoresistive element 11, and an electronic circuit 13 that processes an output signal of the magnetoresistive element 11. 14
.. 15.16 is a streamline indicating the flow direction of the swirling flow, and 1
Reference numerals 7, 18, and 19 are jet ports that eject swirling flows, respectively.

このように構成された従来例において水等の被検出流体
が流量検出装置に満たされると、比重1に近い磁性球体
7は永久磁石12の磁力により第3図に示すように永久
磁石12側に吸引された状態となっている。この様な状
態で被検出流体が図中上矢印側から流入すると、被検出
流体は固定翼5の翼2.3.4で構成された噴出口17
.18.19から旋回流となって流出する。この旋回流
の中に位置する磁性球体7は球体受け9の周回当接面8
に当接し流れの方向に対し垂直方向で周回運動を続ける
。この時、磁性球体7は流量に比例した回転数で周回運
動をする。前記磁性球体7の回転を検出する手段として
は磁気検出により行なっている。
In the conventional example configured as described above, when the flow rate detection device is filled with a fluid to be detected such as water, the magnetic sphere 7 whose specific gravity is close to 1 is moved toward the permanent magnet 12 side by the magnetic force of the permanent magnet 12 as shown in FIG. It is in a state of being absorbed. When the fluid to be detected flows in from the upper arrow side in the figure in such a state, the fluid to be detected flows into the jet port 17 formed by the blades 2.3.4 of the fixed blade 5.
.. It flows out from 18.19 as a swirling flow. The magnetic sphere 7 located in this swirling flow is the orbiting contact surface 8 of the sphere receiver 9.
and continues its circular motion in the direction perpendicular to the flow direction. At this time, the magnetic sphere 7 moves around at a rotational speed proportional to the flow rate. The rotation of the magnetic sphere 7 is detected by magnetic detection.

磁気抵抗素子11の近傍に前記磁気抵抗素子11に一定
の強さの磁界を与える永久磁石12を設けている。
A permanent magnet 12 is provided near the magnetoresistive element 11 to apply a magnetic field of a constant strength to the magnetoresistive element 11.

今、前記磁性球体7が前記磁気抵抗素子11の下方向を
通過すると、前記永久磁石12から前記磁気抵抗素子1
1へ作用している磁界の方向が変化し、前記磁気抵抗素
子11の抵抗値が変化する。この抵抗値の変化を電圧の
変化としてとらえ、パルス信号に変換し出力する。従っ
て磁性球体7が1回転するごとに1パルスの信号が出力
されることになる。
Now, when the magnetic sphere 7 passes below the magnetoresistive element 11, the permanent magnet 12
The direction of the magnetic field acting on the magnetoresistive element 11 changes, and the resistance value of the magnetoresistive element 11 changes. This change in resistance value is interpreted as a change in voltage, converted into a pulse signal, and output. Therefore, one pulse signal is output every time the magnetic sphere 7 rotates once.

発明が解決しようとする課題 しかし、この襟な従来の流量検出装置は始動流量が大き
い、即ち磁性球体7が回転を始める流量が大きくなると
言う欠点があった。その理由は第4図に示す様に磁性球
体7が永久磁石12の磁力により永久磁石側に吸引され
た状態で被検出流体が流れると翼2と翼4で構成される
噴出口から出た旋回流が前記磁性球体7に衝突し、前記
磁性球体7が回転を開始するが、前記永久磁石12の前
記磁性球体7吸引力が大きいため大流量を流し旋回流の
前記磁性球体7への衝突エネルギが前記吸引力を越えな
いと前記磁性球体7が回転しないものであった。従って
流量検出器の最低検出流量が大きくなっていた。
Problems to be Solved by the Invention However, this conventional flow rate detection device has a drawback in that the starting flow rate is large, that is, the flow rate at which the magnetic sphere 7 starts rotating is large. The reason for this is that, as shown in Fig. 4, when the fluid to be detected flows while the magnetic sphere 7 is attracted to the permanent magnet side by the magnetic force of the permanent magnet 12, the fluid flows out from the spout consisting of the blades 2 and 4. The flow collides with the magnetic sphere 7, and the magnetic sphere 7 starts rotating. However, since the magnetic sphere 7 attracting force of the permanent magnet 12 is large, a large flow is caused, and the energy of the swirling flow colliding with the magnetic sphere 7 is reduced. The magnetic sphere 7 would not rotate unless it exceeded the attractive force. Therefore, the minimum detected flow rate of the flow rate detector has become large.

そこで本発明は前記磁性球体が永久磁石側に吸引された
状態においても低流量で前記磁性球体を回転可能とし、
最低検出流量を小さくすることを目的としている。
Therefore, the present invention makes it possible to rotate the magnetic sphere at a low flow rate even when the magnetic sphere is attracted to the permanent magnet side,
The purpose is to reduce the minimum detected flow rate.

課題を解決するための手段 前記課題を解決するために本発明は、流路中を流れる被
検出流体を軸流旋回させる複数翼で構成された複数の噴
出口を有する旋回手段と、前記旋回手段による旋回流の
中に位置し流れの方向に対し垂直で周回する磁性球体と
、前記磁性球体の下流に位置し前記磁性球体の周回当接
面を有する球体受けと、前記流路の外に設けられ永久磁
石の磁界中に設けられた磁気検出素子からなる回転検出
手段とを備え、前記複数の噴出口から噴出される旋回流
のうち前記永久磁石に対向した位置に静止した前記磁性
球体に対し衝突する旋回流の流速が大きくなる様に構成
したものである。
Means for Solving the Problems In order to solve the problems described above, the present invention provides a swirling means having a plurality of ejection ports configured with a plurality of blades for axially swirling the fluid to be detected flowing in a flow path, and the swirling means. a magnetic sphere located in the swirling flow and orbiting perpendicularly to the flow direction; a sphere receiver located downstream of the magnetic sphere and having a circular contact surface for the magnetic sphere; and a sphere receiver provided outside the flow path. rotation detecting means consisting of a magnetic detection element provided in the magnetic field of the permanent magnet, and detecting the rotation of the magnetic sphere stationary at a position facing the permanent magnet among the swirling flows ejected from the plurality of jet ports. It is constructed so that the velocity of the colliding swirling flows is increased.

作用 本発明は上記構成により、静止した磁性球体への衝突エ
ネルギが大きくなるため前記(n性球体が永久磁石側に
吸引された状態においても前記磁性球体の回転開始流量
を小さくすることが出来、低流量検を可能としたもので
ある。
Effect The present invention has the above-mentioned configuration, so that the energy of collision with the stationary magnetic sphere becomes large, so that even when the n-type sphere is attracted to the permanent magnet side, the flow rate at which the magnetic sphere starts rotating can be reduced. This enables low flow rate detection.

実施例 以下、本発明の一実施例を添付図面にもとづいて説明す
る。第1図、第2図において20はハウジングである。
Embodiment Hereinafter, one embodiment of the present invention will be described based on the accompanying drawings. In FIGS. 1 and 2, 20 is a housing.

このハウジング20の内部には流体を旋回流とするため
の複数の翼21.22.23とハブ24で構成される固
定翼25が流路内壁26に密着して設けられている。前
記固定翼25の下流には流路内を周回する磁性球体27
が設けられている。この磁性球体27は内部に磁性金属
中空球を有し外部を樹脂モールドした構成で、水中にお
いての比重はほぼ1に近い磁性球体となっている。この
磁性球体27の下流には前記磁性球体27が下流側へ流
出するのを防止すると共に前記磁性球体27の周回当接
面28を有する球体受け29が設けられている。30.
31.32は複数の翼21.22.23で構成された噴
出口である。またハブ24と翼21の角度αは一定の角
度(例えば50度)で構成されており、ハブ24と翼2
2の角度も前記ハブ24と翼21の角度と同角度に構成
している。しかしハブ24と翼23の角度は前述の角度
に比べて大きく(例えば70度)構成されている。従っ
て噴出口30の面積に比べ他の噴出口31.32の面積
は小さく構成されることになる。尚ハウジング20の外
部には前記磁性球体27の回転を検出する検出器33が
設けられている。この検出器33は磁気抵抗素子34と
この磁気抵抗素子34に磁界を与える永久fj!石35
と前記磁気抵抗素子34の信号を処理する電子回路36
が設けられている。37.38.39は旋回流の流れ方
向を示す流線である。この様に構成された本発明におい
て水等の流体が流量検出装置に満たされると、比重1に
近い磁性球体27は永久磁石35の磁力により前記永久
磁石35側に吸引された状態となる。この様な状態で被
検出流体が図中上矢印側から流入すると被検出流体は固
定翼25の噴出口30.31.32から噴出され旋回流
を構成する。
Inside the housing 20, fixed blades 25 made up of a plurality of blades 21, 22, 23 and a hub 24 for creating a swirling flow of fluid are provided in close contact with the inner wall 26 of the flow path. A magnetic sphere 27 orbiting in the flow path is downstream of the fixed blade 25.
is provided. The magnetic sphere 27 has a hollow magnetic metal sphere inside and a resin molded outside, and has a specific gravity close to 1 in water. A sphere receiver 29 is provided downstream of the magnetic sphere 27 to prevent the magnetic sphere 27 from flowing out to the downstream side and has a rotating contact surface 28 for the magnetic sphere 27 . 30.
Reference numeral 31.32 is a jet nozzle composed of a plurality of blades 21.22.23. Further, the angle α between the hub 24 and the blade 21 is a constant angle (for example, 50 degrees), and the angle α between the hub 24 and the blade 21 is
The angle 2 is also configured to be the same as the angle between the hub 24 and the blade 21. However, the angle between the hub 24 and the blades 23 is larger (for example, 70 degrees) than the above-mentioned angle. Therefore, the areas of the other jet ports 31 and 32 are configured to be smaller than the area of the jet port 30. A detector 33 for detecting the rotation of the magnetic sphere 27 is provided outside the housing 20. This detector 33 includes a magnetoresistive element 34 and a permanent fj! which applies a magnetic field to this magnetoresistive element 34. stone 35
and an electronic circuit 36 for processing the signals of the magnetoresistive element 34.
is provided. 37, 38, and 39 are streamlines indicating the flow direction of the swirling flow. In the present invention configured in this manner, when the flow rate detection device is filled with a fluid such as water, the magnetic sphere 27 whose specific gravity is close to 1 is attracted to the permanent magnet 35 side by the magnetic force of the permanent magnet 35. When the fluid to be detected flows in from the upper arrow side in the figure in such a state, the fluid to be detected is ejected from the jet ports 30, 31, and 32 of the fixed blade 25, forming a swirling flow.

この旋回流は前記永久磁石35に吸引され静止している
磁性球体27に衝突し前記磁性球体27を回転運動させ
ることになる。本実施例においてはハブ24と翼23の
角度αを他の翼21.22とハブ24の角度αに比べ大
きくしているため噴出口31.32の面積は、噴出口3
0に比べ小さく構成されている。従って永久磁石35に
対向した位置に静止した磁性球体27に対し衝突する旋
回流を噴出する噴出口31の流速は他の噴出口30から
噴出する流速に比べ速くなり、前記磁性球体27への衝
突エネルギが大きくなるため低流量で前記磁性球体27
が回転を開始する。回転している磁性球体27の検出方
法は磁気検出によっている。即ち周回している磁性球体
27が前記磁気抵抗素子34の下方向を通過すると前記
永久磁石35から前記磁気抵抗素子34へ作用している
磁界の方向が変化し、前記6イ1気抵抗素子34の抵抗
値が変化する。この抵抗値の変化を電圧の変化としてと
らえ、パルス信号に変換し出力する。従って磁性球体2
7が1回転するごとにlパルスの信号が出力されること
になる。
This swirling flow is attracted by the permanent magnet 35 and collides with the stationary magnetic sphere 27, causing the magnetic sphere 27 to rotate. In this embodiment, since the angle α between the hub 24 and the blade 23 is larger than the angle α between the other blades 21.22 and the hub 24, the area of the jet nozzle 31.32 is
It is configured smaller than 0. Therefore, the flow velocity of the jet nozzle 31 that spouts out a swirling flow that collides with the magnetic sphere 27 stationary at a position facing the permanent magnet 35 is faster than the flow velocity of the jet from the other jet nozzles 30, and the flow speed that collides with the magnetic sphere 27 increases. Because the energy increases, the magnetic sphere 27
starts rotating. The rotating magnetic sphere 27 is detected by magnetic detection. That is, when the orbiting magnetic sphere 27 passes below the magnetic resistance element 34, the direction of the magnetic field acting from the permanent magnet 35 to the magnetic resistance element 34 changes, and the magnetic resistance element 34 resistance value changes. This change in resistance value is interpreted as a change in voltage, converted into a pulse signal, and output. Therefore, magnetic sphere 2
A signal of 1 pulse is output every time 7 rotates once.

本実施例においては、複数の翼の内で1枚の翼のf’I
ji斜角度を変えるだけの構成であるため、低圧…で磁
性球体27の始動流量を小さくすることができる。また
簡単な構成であるため安価に製造することが出来ると言
う効果を有するものである。
In this embodiment, f'I of one wing among a plurality of wings is
Since the configuration is such that only the angle of inclination is changed, the starting flow rate of the magnetic sphere 27 can be reduced at low pressure. Furthermore, since it has a simple configuration, it has the advantage that it can be manufactured at low cost.

発明の効果 以上のように本発明の流量検出装置は流路中を流れる被
検出流体を軸流旋回させる複数の翼で構成された複数の
噴出口を有する旋回手段と、前記旋回手段による旋回流
の中に位置し流れの方向に対し垂直面で周回する磁性球
体と、前記磁性球体の下流に位置し前記磁性球体の周回
当接面を有する球体受けと、前記流路の外に設けられた
永久磁石の磁界中に設けられた磁気検出素子からなる回
転検出手段とを備え、前記複数の噴出口から噴出される
旋回流の内前記永久磁石に対向した位置に静止した前記
磁性球体に対し衝突する旋回流の流速を大きくすること
により、低流量が流れた時においても、磁性球体に衝突
する衝突エネルギが大きくなるため、磁性球体が永久磁
石側に吸引された状態であっても、磁性球体は容易に周
回する。
Effects of the Invention As described above, the flow rate detection device of the present invention includes a swirling means having a plurality of jet ports each formed of a plurality of blades for axially swirling the detected fluid flowing in a flow path, and a swirling flow generated by the swirling means. a magnetic sphere located in the flow path and orbiting in a plane perpendicular to the flow direction; a sphere receiver located downstream of the magnetic sphere and having a rotating contact surface for the magnetic sphere; and a sphere receiver provided outside the flow path. rotation detection means consisting of a magnetic detection element provided in the magnetic field of a permanent magnet, and among the swirling flows ejected from the plurality of jet ports, collision occurs with the magnetic sphere stationary at a position facing the permanent magnet. By increasing the flow velocity of the swirling flow, even when a low flow rate flows, the collision energy that collides with the magnetic sphere increases, so even if the magnetic sphere is attracted to the permanent magnet side, the magnetic sphere easily orbits.

従って低流量検出が可能となり、流量検出装置としては
広いレンジの流量計測が可能となる。
Therefore, it is possible to detect a low flow rate, and the flow rate detection device can measure a wide range of flow rates.

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

第1図は本発明の一実施例を示す2iHt検出装置の断
面図、第2図は第1図の横断面図、第3図は従来例にお
ける流量検出装置の断面図、第4図は第3図の横断面図
である。 21、22..23・・・・・・翼、25・・・・・・
旋回手段(固定翼)、27・・・・・・磁性球体、28
・・・・・・周回当接面、29・・・・・・球体受け、
30.31.32・・・・・・噴出口、34・・・・・
・磁気検出素子、35・・・・・・永久磁石。
FIG. 1 is a sectional view of a 2iHt detection device showing an embodiment of the present invention, FIG. 2 is a cross-sectional view of FIG. 1, FIG. 3 is a sectional view of a conventional flow rate detection device, and FIG. FIG. 3 is a cross-sectional view of FIG. 21, 22. .. 23...Tsubasa, 25...
Rotating means (fixed wing), 27...Magnetic sphere, 28
... Circumferential contact surface, 29 ... Ball receiver,
30.31.32... spout, 34...
・Magnetic detection element, 35...Permanent magnet.

Claims (3)

【特許請求の範囲】[Claims] (1)流路中を流れる被検出流体を軸流旋回させる複数
の翼で構成された複数の噴出口を有する旋回手段と、前
記旋回手段による旋回流の中に位置し流れの方向に対し
垂直面で周回する磁性球体と、前記磁性球体の下流に位
置し前記磁性球体の周回当接面を有する球体受けと、前
記流路の外に設けられ永久磁石の磁界中に設けられた磁
気検出素子からなる回転検出手段とを備え、前記複数の
噴出口から噴出される旋回流のうち、前記永久磁石に対
向した位置に静止した前記磁性球体に対し衝突する旋回
流の流速を大きくした流量検出装置。
(1) A swirling means having a plurality of jet ports made of a plurality of blades that axially swirls the fluid to be detected flowing in a flow path, and a swirling means located in the swirling flow caused by the swirling means and perpendicular to the direction of the flow. a magnetic sphere orbiting in a plane, a sphere receiver located downstream of the magnetic sphere and having a rotating contact surface for the magnetic sphere, and a magnetic detection element provided outside the flow path and in the magnetic field of the permanent magnet. A flow rate detection device that increases the flow velocity of the swirling flow that collides with the magnetic sphere stationary at a position facing the permanent magnet among the swirling flows ejected from the plurality of jet ports. .
(2)磁性球体に対し衝突する旋回流の噴出口の面積を
他の噴出口の面積に比べ小さくした特許請求の範囲第1
項記載の流量検出装置。
(2) Claim 1 in which the area of the jet of the swirling flow colliding with the magnetic sphere is smaller than the area of other jets.
Flow rate detection device as described in section.
(3)複数の翼のうち、少なくとも1枚の翼の傾斜角度
を変えて成る特許請求の範囲第1項記載の流量検出装置
(3) The flow rate detection device according to claim 1, wherein the inclination angle of at least one of the plurality of blades is changed.
JP14593889A 1989-06-08 1989-06-08 Flow rate detector Expired - Fee Related JPH0765912B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14593889A JPH0765912B2 (en) 1989-06-08 1989-06-08 Flow rate detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14593889A JPH0765912B2 (en) 1989-06-08 1989-06-08 Flow rate detector

Publications (2)

Publication Number Publication Date
JPH0310118A true JPH0310118A (en) 1991-01-17
JPH0765912B2 JPH0765912B2 (en) 1995-07-19

Family

ID=15396535

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14593889A Expired - Fee Related JPH0765912B2 (en) 1989-06-08 1989-06-08 Flow rate detector

Country Status (1)

Country Link
JP (1) JPH0765912B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US11186265B2 (en) 2017-07-13 2021-11-30 Honda Motor Co., Ltd. Method and device for collecting and supplying brake fluid

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US11186265B2 (en) 2017-07-13 2021-11-30 Honda Motor Co., Ltd. Method and device for collecting and supplying brake fluid

Also Published As

Publication number Publication date
JPH0765912B2 (en) 1995-07-19

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