JP4135432B2 - Flow measuring device - Google Patents
Flow measuring device Download PDFInfo
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- JP4135432B2 JP4135432B2 JP2002229726A JP2002229726A JP4135432B2 JP 4135432 B2 JP4135432 B2 JP 4135432B2 JP 2002229726 A JP2002229726 A JP 2002229726A JP 2002229726 A JP2002229726 A JP 2002229726A JP 4135432 B2 JP4135432 B2 JP 4135432B2
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Description
【0001】
【発明の属する技術分野】
本発明は、ガスなどの流量を計測する流量計測装置に関するものである。
【0002】
【従来の技術】
従来のこの種の流量計測装置を、図5に基づいて説明する。図において、流体通路1の一部に超音波式のような流量検出手段2を備えて流量を計測する。流れに周期的な変動がある場合には、計測のタイミングによって流量測定値にバラツキが生じる。例えば家庭用ガス消費量を計量するガスメータでは、近くでガスエンジンが運転されると圧力変動が発生する。このため圧力変動を緩衝するため弁体3を有する脈動吸収装置4を設け脈動レベルを低減することが行われていた。
【0003】
【発明が解決しようとする課題】
しかしながら従来の流量計測装置では、脈動吸収装置4によって生じる流れの乱れや流速分布の偏りが流量計測の精度を悪化させる欠点があった。また弁体が開いた時の隙間による透過は面積Sの隔壁にその弁体の面積の1/nの隙間があるとすると透過損失TLは、
TL≒101ogn
たとえば、隙間が1/1000あるときには透過損失は30db以上にはならない。
【0004】
またガスエンジンが運転された時の流体通路の空洞共振現象に対して通常問題になるのは50HZ〜150HZの周波数であるが、空洞共振に対し流体通路形状を変更し、その共振周波数を変更したり、腹になる位置を移動させようということはまず困難である。
【0005】
本発明はかかる従来の課題に鑑み、弁体等の可動部を有せず圧力変動耐性を向上する流量計測装置を提供することを目的とする。
【0006】
【課題を解決するための手段】
本発明は、上記課題を解決するために、入口通路と出口通路に直交して配置された流体通路と、前記流体通路内に配置され通路の流量を検出する流量検出手段と、前記流体通路の上流側に、入口通路断面と同等以上の断面積を有し、入口からの流体の導入方向の延長線上で、前記流体通路と交差し前記流体通路の高さの1〜5倍の深さを有する凹部とを備え、前記流体通路の一端に設けた凹部に吸音部材を設けたものである。
【0007】
上記発明によって圧力変動を抑制するとともに、脈動を吸収し正確な流量を求める。
【0008】
【発明の実施の形態】
本発明は、入口通路と出口通路に直交して配置された流体通路と、前記流体通路内に配置され通路の流量を検出する流量検出手段と、前記流体通路の上流側に、入口通路断面と同等以上の断面積を有し、入口からの流体の導入方向の延長線上で、前記流体通路と交差し前記流体通路の高さの1〜 5 倍の深さを有する凹部とを備え、前記流体通路の一端に設けた凹部に吸音部材を設けたもので、脈動がある場合にはその脈動を吸収し、流れの乱れを発生させず流量を正確に計測する。吸音部材表面は楔状の凹凸を有し、さらに吸音性を高める。
【0009】
また、吸音部材として微細セル構造を有する多孔質発泡体を備えたもので、この多孔質部材によって脈動を吸収し流量計測を安定化させるものである。
【0010】
また、吸音部材としてバルク状部材を備えたもので、この繊維状部材の密度を小さくすることによって脈動を吸収し流量計測を安定化させるものである。
【0011】
【実施例】
以下、本発明の実施例について図面を用いて説明する。
【0012】
(実施例1)
図1は本発明の実施例1の流量計測装置を示した構成図である。図1において、流体通路5に流量検出手段6を設け通路の流量を検出する。流量検出手段6は流れの上流側と下流側に超音波送受信器6aと6bをそれぞれ配置し、上流から下流への超音波の伝搬時間と、下流から上流への超音波伝搬時間の時間差から流量を算出するもので、詳細は後述する。流量検出手段6の上流5aには流体通路の高さの1〜5倍の深さを有する凹部7aが設けられている。凹部7aには吸収部材7bが設けられ圧力変動吸収部7を構成している。吸収部材7bは、前記凹部7aに吸収部材7bの弾性を利用して圧入、固着される。吸収部材7bの上端面は、流体通路下端より流体通路高さhの1/5〜1低く設けてあり曲がり部を通過する際の圧力損失を低減している。吸収部材7bにより圧力変動抑制効果がさらに大きくなる。圧力変動が発生した場合流れは瞬間的に凹部7aに流れ込む迂回流を起こすが前記吸収部材7bにより凹部7aに流れ込む迂回流を抑制し効果的に圧力変動を吸収することができる。
【0013】
次に動作について述べる。図1において圧力変動吸収部7は流量検出手段6の上流側に設けられており、入口からの流体の流れの延長線上でかつ計測流路に交差するように構成されている。入口から出口に順方向に流体が流れると小流量の場合には、前記凹部7aに回り込む流れは無くほぼ最短の流線を描く。凹部7aは流体通路の高さの1〜5倍の深さとしている。1倍以下では圧力変動を吸収する効果が小さく5倍以上にしても効果の増加が認められない。流れがないときには圧力脈動は凹部7aによって吸収されるため、圧力は大きく増加しない。圧力変動によって出口から入口に逆方向の流れが発生すると、凹部7aで圧力上昇を緩和する。
【0014】
すなわち流体通路5に流れがない場合や小流量の場合には、圧力変動によって発生する逆流を緩和し、また順方向の流れも圧力変動吸収部7によって抑制され、脈動的な流れは低減され、流量検出手段6の値も大きく変動せず、平均流量を算出できる。また、流体通路5に大流量が流れ、このとき圧力変動が発生すると圧力変動を抑制する効果が小さいので流量誤差を発生するが、平均流量が大きく流れており、相対的に誤差の比率は小さいので問題にならない。
【0015】
圧力変動吸収部7を流量検出手段6より上流側に設けると、この部分で圧力変動が抑制されるので、流量検出手段6には脈動の影響がよりいっそう小さくなる。
【0016】
一方上流に圧力変動吸収部7が設けられることによって流れが変化し流量精度を悪化させることが考えられる。しかし、流体は前記凹部7aに回り込むわけではなく平均して流れるので、流量検出手段6への影響は極めて小さい。
【0017】
図2は超音波による流量検出手段の詳細を示したものである。図2において、第1送受信器6aと送受信する第2送受信器6bが流れ方向に配置されている。8は超音波に基づく信号を処理し演算する流量演算手段で、9は送信回路で、トリガ手段10によって第1送受信器6aを駆動し、第2送受信器6bに向け、すなわち上流から下流に超音波を送信する。増幅回路11は第2送受信器6bで受信した信号を増幅し、この増幅された信号は基準信号と比較回路12で比較され、基準信号以上の信号が検出された後、繰り返し手段13で再度トリガ手段10から送信が行われ、上記の送受信を所定の回数を繰り返した後の時間をタイマカウンタのような計時手段14で求める。
【0018】
次に切換手段15で第1送受信器6aと第2送受信器6bの送受信を切り換えて、第2送受信器6bから第1送受信器6aすなわち下流から上流に向かって超音波信号を送信し、この送信を前述のように繰り返し、その時間を計時する。
【0019】
そして、その時間差から管路の大きさや流れの状態を考慮して流量演算手段8で流量値を求める。
【0020】
(実施例2)
図3は本発明の実施例を示す構成図で、流体通路5に設けられた流量検出手段6の上流側に凹部7aと吸収部材7bからなる圧力変動吸収部7および下流側に凹部16aと吸収部材16bからなる圧力変動吸収部16が設けられている。
【0021】
次に動作について述べる。流れがないときには出口側から脈動が加わった場合、圧力変動吸収部16はその脈動を吸収し圧力は大きく増加しない。圧力変動によって局部的な逆方向の流れが発生しても、圧力変動吸収部16によって流れが減少される。圧力変動吸収部16は流量検出手段6の下流側にあるので、この部分で多少流れが乱れても流量検出に悪影響を及ぼすことがない。
【0022】
(実施例3)
図3において吸収部材7b、16bは多孔質発泡体を設けたもので、小流量時にはこの多孔質が圧力変動を吸収するため流れは極めて安定である。また多孔質発泡体を多層にし流体に接する側7d、16dの表面の密度を小さくすることにより吸収応答性が高く流量検出精度が高くなる。流体に接する表面の層7d、16dは、音響インピーダンスが気体に近く密度が小さい方が好ましい。
【0023】
(実施例4)
図3において吸収部材7b、16bは微細なセル構造を有する多孔質発泡体を設けたもので、セルの大きさは超音波の波長の1/4〜1が好ましい。
【0024】
(実施例5)
図4において吸音材はバルク状部材17b、18bとしたもので、小流量時にはこのバルク状部材の空隙が圧力変動を吸収するため流れが安定する。またバルク状部材は中心が中空になったミクロチューブ状の中空繊維にし密度を小さくすることにより吸収応答性が高くなる。特に流体に接する側の表面は、音響インピーダンスが気体に近く密度が小さくなるよう繊維の密度が小さい方が好ましい。
【0025】
(実施例6)
図1において吸収部材7bの端面に楔状の凹凸を複数形成している。吸収部材7bは、楔状の凹部において吸収、反射を繰り返すことにより減衰しさらに圧力変動が抑制される。
【0026】
以上の説明から明らかなようにこれまで説明した各実施例によれば、次の効果が得られる。
【0027】
(1) 実施例の流量測定装置によれば、流体通路5と、前記流体通路5の流量を
検出する流量検出手段6と、前記流体通路5の上流側に圧力変動を抑制する凹部7aとを備えたので、脈動がある場合にはその脈動を吸収し、脈動がない場合にも流れの乱れを発生させず流量を正確に計測できる。
【0028】
さらに前記凹部7aに設けた吸音部材7bにより圧力変動を吸収するので、脈動がなく流れの安定性をより一層高めることができる。
【0029】
(2)さらに、流体通路5と、前記流体通路5の流量を検出する流量検出手段6と、前記流体通路5の上流側および下流側に、圧力変動を抑制するとともに吸音部材7b,16bを収容する凹部7a,16aとを備えたので逆方向の流れを抑制するとともに順方向には、圧力変動を抑制する下流側凹部16aでの流れの乱れによる流量計測精度への影響が少なく、高精度に計測できる。さらに上流側と下流側を対称形状にすることにより圧力変動の影響が相殺され流量計測精度への影響をさらに少なくすることができる。
【0030】
(3)また、吸音部材7b,16bは多孔質発泡体としたので脈動がなく流れの安定性を高めることができ計測精度が高い。
【0031】
(4)吸音部材7b,16bは微細セル構造を有する多孔質発泡体としたのでさらに圧力変動吸収が高まり脈動がなく流れの安定性を高めることができ計測精度が高い。
【0032】
(5)吸音部材7b,16bをバルク状部材により構成したので、繊維の密度を小さくでき、低流量時にも圧力変動による流れの乱れが小さく、高精度に計測できる。
【0033】
(6)また該吸音部材7bの表面には楔状突起を有し、楔状突起間で吸収、反射を繰り返すため吸音率が大きくなり脈動がなく流れの安定性をより一層高めることができ計測精度が高い。
【0034】
【発明の効果】
本発明によれば、精度よく流量測定ができるものである。
【図面の簡単な説明】
【図1】 本発明の実施例1、実施例6の流量計測装置の構成図
【図2】 同装置における流量計測手段のブロック図
【図3】 本発明の実施例2の流体通路の上流側および下流側に設けた凹部と吸収部材、実施例3、4の微細セル構造を有する多孔質発泡体を示す構成図
【図4】 本発明の実施例5のバルク状部材の構成図
【図5】 従来の脈動吸収装置の構成図
【符号の説明】
5 流体通路
6 流量検出手段
7 変動圧力吸収部
7a 凹部
7b 吸収部材[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a flow rate measuring device for measuring a flow rate of gas or the like.
[0002]
[Prior art]
A conventional flow measuring device of this type will be described with reference to FIG. In the figure, a flow rate detecting means 2 such as an ultrasonic type is provided in a part of the fluid passage 1 to measure the flow rate. When there is a periodic fluctuation in the flow, the flow rate measurement value varies depending on the measurement timing. For example, in a gas meter that measures household gas consumption, pressure fluctuation occurs when a gas engine is operated nearby. For this reason, in order to buffer the pressure fluctuation, a pulsation absorbing device 4 having a valve body 3 is provided to reduce the pulsation level.
[0003]
[Problems to be solved by the invention]
However, the conventional flow rate measuring device has a drawback that the flow turbulence caused by the pulsation absorbing device 4 and the deviation of the flow velocity distribution deteriorate the accuracy of the flow rate measurement. Further, when the valve body is opened, the transmission through the gap is assumed to be 1 / n of the area of the valve body in the partition wall of the area S.
TL ≒ 101ogn
For example, when the gap is 1/1000, the transmission loss does not exceed 30 db.
[0004]
Moreover, the frequency of 50HZ to 150HZ is usually a problem for the cavity resonance phenomenon of the fluid passage when the gas engine is operated. However, the shape of the fluid passage is changed for the cavity resonance, and the resonance frequency is changed. It is difficult to move the position to become a stomach.
[0005]
The present invention has been made in view of the conventional problems, and an object of the present invention is to provide a flow rate measuring device that does not have a movable part such as a valve body and improves pressure fluctuation resistance.
[0006]
[Means for Solving the Problems]
The present invention, in order to solve the above problems, a fluid passage disposed orthogonally to the inlet passage and an outlet passage, a flow rate detecting means for detecting the flow rate of the passage being disposed in said fluid passage, said fluid passage On the upstream side, it has a cross-sectional area equal to or larger than the cross section of the inlet passage, and intersects the fluid passage on the extension line in the direction of introduction of fluid from the inlet, and has a depth of 1 to 5 times the height of the fluid passage. A sound absorbing member is provided in a recess provided at one end of the fluid passage .
[0007]
The above invention suppresses pressure fluctuations and absorbs pulsation to obtain an accurate flow rate.
[0008]
DETAILED DESCRIPTION OF THE INVENTION
The present invention includes a fluid passage disposed orthogonally to the inlet passage and an outlet passage, a flow rate detecting means for detecting the flow rate of the passage being disposed in said fluid passage, upstream of the fluid passage, an inlet passage section A concave portion having a cross-sectional area equal to or greater than that and extending in the direction of introduction of fluid from the inlet and intersecting with the fluid passage and having a depth of 1 to 5 times the height of the fluid passage. A sound absorbing member is provided in a recess provided at one end of the passage, and when there is pulsation, the pulsation is absorbed and the flow rate is accurately measured without causing flow disturbance. The surface of the sound absorbing member has wedge-shaped irregularities and further enhances sound absorption.
[0009]
In addition, a porous foam having a fine cell structure is provided as a sound absorbing member, and the pulsation is absorbed by this porous member to stabilize the flow rate measurement.
[0010]
Further, a bulk member is provided as a sound absorbing member, and by reducing the density of the fibrous member, pulsation is absorbed and flow measurement is stabilized.
[0011]
【Example】
Embodiments of the present invention will be described below with reference to the drawings.
[0012]
(Example 1)
FIG. 1 is a configuration diagram illustrating a flow rate measuring apparatus according to a first embodiment of the present invention. In FIG. 1, a flow rate detecting means 6 is provided in the fluid passage 5 to detect the flow rate of the passage. The flow rate detection means 6 is arranged with ultrasonic transmitters / receivers 6a and 6b on the upstream side and downstream side of the flow, respectively, and the flow rate is determined from the time difference between the ultrasonic propagation time from upstream to downstream and the ultrasonic propagation time from downstream to upstream. The details will be described later. A recess 7a having a depth of 1 to 5 times the height of the fluid passage is provided in the upstream 5a of the flow rate detection means 6. The recess 7a is provided with an absorbing member 7b to constitute the pressure fluctuation absorbing portion 7. The absorbing member 7b is press-fitted and fixed to the recess 7a using the elasticity of the absorbing member 7b . The upper end surface of the absorbing member 7b is provided to be 1/5 to 1 lower than the fluid passage height h from the lower end of the fluid passage to reduce pressure loss when passing through the bent portion. The pressure fluctuation suppressing effect is further increased by the absorbing member 7b. When a pressure fluctuation occurs, the flow momentarily causes a detour flow that flows into the recess 7a , but the absorbing member 7b suppresses the detour flow that flows into the recess 7a and can effectively absorb the pressure variation.
[0013]
Next, the operation will be described. In FIG. 1, the pressure fluctuation absorbing portion 7 is provided on the upstream side of the flow rate detecting means 6, and is configured to extend on the extension line of the fluid flow from the inlet and intersect the measurement flow path. When the fluid flows in the forward direction from the inlet to the outlet, in the case of a small flow rate, there is no flow that wraps around the concave portion 7a, and an almost shortest streamline is drawn. The recess 7a has a depth that is 1 to 5 times the height of the fluid passage. If it is less than 1 time, the effect of absorbing pressure fluctuation is small, and even if it is 5 times or more, an increase in effect is not recognized. When there is no flow, the pressure pulsation is absorbed by the recess 7a , so the pressure does not increase greatly. When a flow in the opposite direction is generated from the outlet to the inlet due to pressure fluctuation, the pressure rise is mitigated by the recess 7a .
[0014]
That is, when there is no flow in the fluid passage 5 or when the flow rate is small, the backflow generated by the pressure fluctuation is relaxed, and the forward flow is also suppressed by the pressure fluctuation absorbing portion 7, and the pulsating flow is reduced. The value of the flow rate detection means 6 does not vary greatly, and the average flow rate can be calculated. Also, if a large flow rate flows through the fluid passage 5 and a pressure fluctuation occurs at this time, the effect of suppressing the pressure fluctuation is small, so a flow rate error occurs. However, the average flow rate is large, and the error ratio is relatively small. So it doesn't matter.
[0015]
When the pressure fluctuation absorbing portion 7 is provided on the upstream side of the flow rate detecting means 6, the pressure fluctuation is suppressed in this portion, so that the influence of pulsation is further reduced on the flow rate detecting means 6.
[0016]
On the other hand, it is conceivable that the flow changes due to the provision of the pressure fluctuation absorber 7 upstream, thereby deteriorating the flow rate accuracy. However, since the fluid does not go around the recess 7a but flows on average, the influence on the flow rate detection means 6 is extremely small.
[0017]
FIG. 2 shows details of the flow rate detecting means using ultrasonic waves. In FIG. 2, the 2nd transmitter / receiver 6b which transmits / receives with the 1st transmitter / receiver 6a is arrange | positioned in the flow direction. 8 is a flow rate calculation means for processing and calculating a signal based on the ultrasonic wave, and 9 is a transmission circuit, which drives the first transmitter / receiver 6a by the trigger means 10 toward the second transmitter / receiver 6b, that is, from upstream to downstream. Send sound waves. The amplifier circuit 11 amplifies the signal received by the second transmitter / receiver 6b. The amplified signal is compared with the reference signal by the comparison circuit 12, and after the signal equal to or higher than the reference signal is detected, the repeater 13 triggers again. Transmission is performed from the means 10, and the time after the above transmission / reception is repeated a predetermined number of times is obtained by the time measuring means 14 such as a timer counter.
[0018]
Next, the switching means 15 switches the transmission / reception of the first transmitter / receiver 6a and the second transmitter / receiver 6b to transmit an ultrasonic signal from the second transmitter / receiver 6b toward the first transmitter / receiver 6a, that is, from downstream to upstream. Is repeated as described above, and the time is counted.
[0019]
Then, the flow rate calculation means 8 obtains the flow value from the time difference in consideration of the size of the pipeline and the flow state.
[0020]
(Example 2)
FIG. 3 is a block diagram showing an embodiment of the present invention, in which the pressure fluctuation absorbing portion 7 composed of the concave portion 7a and the absorbing member 7b on the upstream side of the flow rate detecting means 6 provided in the fluid passage 5 and the concave portion 16a on the downstream side are absorbed. A pressure fluctuation absorbing portion 16 composed of the member 16b is provided.
[0021]
Next, the operation will be described. When there is no flow, if a pulsation is applied from the outlet side, the pressure fluctuation absorber 16 absorbs the pulsation and the pressure does not increase greatly. Even if a local reverse flow occurs due to the pressure fluctuation, the flow is reduced by the pressure fluctuation absorber 16 . Since the pressure fluctuation absorber 16 is located downstream of the flow rate detection means 6, even if the flow is somewhat disturbed in this portion, the flow rate detection is not adversely affected.
[0022]
(Example 3)
In FIG. 3, the absorbent members 7b and 16b are provided with a porous foam, and the flow is extremely stable when the flow rate is small because the porous body absorbs pressure fluctuations. Further, by making the porous foam into a multilayer and reducing the density of the surfaces 7d and 16d in contact with the fluid, the absorption response is high and the flow rate detection accuracy is high. It is preferable that the surface layers 7d and 16d in contact with the fluid have an acoustic impedance close to that of gas and have a low density.
[0023]
Example 4
In FIG. 3, the absorbing members 7b and 16b are provided with a porous foam having a fine cell structure, and the size of the cell is preferably 1/4 to 1 of the wavelength of the ultrasonic wave.
[0024]
(Example 5)
In FIG. 4, the sound-absorbing material is bulky members 17b and 18b, and when the flow rate is small, the air flow in the bulky member absorbs pressure fluctuations and the flow is stabilized. Further, the bulk-like member has a micro tube-like hollow fiber with a hollow center, and the density is reduced to increase the absorption response. In particular, the surface on the side in contact with the fluid preferably has a low fiber density so that the acoustic impedance is close to that of gas and the density is low.
[0025]
(Example 6)
In FIG. 1, a plurality of wedge-shaped irregularities are formed on the end face of the absorbing member 7b. The absorbing member 7b is attenuated by repeating absorption and reflection in the wedge-shaped recess, and pressure fluctuation is further suppressed.
[0026]
As is clear from the above description, according to each of the embodiments described so far, the following effects can be obtained.
[0027]
(1) according to the flow rate measuring apparatus of the embodiment, the fluid passage 5, the flow rate detecting means 6 for detecting the flow rate of the fluid passage 5, and suppressing recess 7a of the pressure fluctuations on the upstream side of the fluid passage 5 Since it is provided, when there is pulsation, the pulsation is absorbed, and even when there is no pulsation, the flow rate can be accurately measured without causing flow disturbance.
[0028]
Further, since the pressure fluctuation is absorbed by the sound absorbing member 7b provided in the concave portion 7a, there is no pulsation and the flow stability can be further enhanced.
[0029]
Housing (2) further includes a fluid passage 5, the flow rate detecting means 6 for detecting the flow rate of the fluid passage 5, the upstream and downstream of the fluid passage 5, the sound absorbing member 7b is suppressed pressure fluctuations, 16b Since the concave portions 7a and 16a are provided, the flow in the downstream side 16a that suppresses the flow in the reverse direction while suppressing the flow in the reverse direction is less affected by the flow disturbance in the downstream concave portion 16a and is highly accurate. It can be measured. Furthermore, by making the upstream side and the downstream side symmetrical, the influence of the pressure fluctuation is offset and the influence on the flow rate measurement accuracy can be further reduced.
[0030]
(3) Further, since the sound absorbing members 7b and 16b are made of a porous foam, there is no pulsation, the flow stability can be improved, and the measurement accuracy is high.
[0031]
(4) Since the sound absorbing members 7b and 16b are made of a porous foam having a fine cell structure, absorption of pressure fluctuation is further increased, there is no pulsation, flow stability can be improved, and measurement accuracy is high.
[0032]
(5) Since the sound absorbing members 7b and 16b are constituted by bulk-like members, the density of the fibers can be reduced, and the flow disturbance due to the pressure fluctuation can be reduced even at a low flow rate, and measurement can be performed with high accuracy.
[0033]
(6) The surface of the sound-absorbing member 7b has wedge-shaped projections, and since absorption and reflection are repeated between the wedge-shaped projections, the sound absorption rate increases, there is no pulsation, flow stability can be further improved, and measurement accuracy is improved. high.
[0034]
【The invention's effect】
According to the present invention, the flow rate can be accurately measured.
[Brief description of the drawings]
FIG. 1 is a block diagram of a flow rate measuring device according to a first embodiment and a sixth embodiment of the present invention. FIG. 2 is a block diagram of a flow rate measuring means in the same device. FIG. 3 is an upstream side of a fluid passage according to a second embodiment of the present invention. FIG. 4 is a configuration diagram showing a porous foam having a concave portion and an absorbing member provided on the downstream side, and a fine cell structure of Examples 3 and 4. FIG. 4 is a configuration diagram of a bulk-like member of Example 5 of the present invention. ] Configuration of conventional pulsation absorber [Explanation of symbols]
5 Fluid passage 6 Flow rate detection means 7 Fluctuating pressure absorbing part 7a Recessed part 7b Absorbing member
Claims (5)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2002229726A JP4135432B2 (en) | 2002-08-07 | 2002-08-07 | Flow measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2002229726A JP4135432B2 (en) | 2002-08-07 | 2002-08-07 | Flow measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JP2004069519A JP2004069519A (en) | 2004-03-04 |
| JP4135432B2 true JP4135432B2 (en) | 2008-08-20 |
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| JP2002229726A Expired - Fee Related JP4135432B2 (en) | 2002-08-07 | 2002-08-07 | Flow measuring device |
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Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2010071944A (en) * | 2008-09-22 | 2010-04-02 | Yazaki Corp | Gas meter |
| CN103470898B (en) * | 2013-09-26 | 2015-06-17 | 苏州优德通力电气有限公司 | Water pipe with water flow direction distinguishing function |
| NL2036242B1 (en) * | 2023-11-10 | 2025-05-20 | Liaoning Sc Tech Co Ltd | Flow stabilizing apparatus for ultrasonic flowmeter and flow stabilizing ultrasonic flowmeter apparatus |
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