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JP7599147B2 - Physical Quantity Measuring Devices - Google Patents
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JP7599147B2 - Physical Quantity Measuring Devices - Google Patents

Physical Quantity Measuring Devices Download PDF

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JP7599147B2
JP7599147B2 JP2020214487A JP2020214487A JP7599147B2 JP 7599147 B2 JP7599147 B2 JP 7599147B2 JP 2020214487 A JP2020214487 A JP 2020214487A JP 2020214487 A JP2020214487 A JP 2020214487A JP 7599147 B2 JP7599147 B2 JP 7599147B2
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receding
wall
flow path
fluid
main flow
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JP2022100485A (en
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真人 佐藤
基之 名和
裕治 中林
正誉 松田
麻子 三好
裕也 高倉
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Panasonic Intellectual Property Management Co Ltd
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Description

本発明は、流動する使用流体の一部をサンプリングして、流体に含まれる成分の濃度等の特性を計測するための構成に関するものである。 The present invention relates to a configuration for sampling a portion of a flowing fluid to measure characteristics such as the concentration of components contained in the fluid.

流路を流れる流体の流れの乱れの影響を受けることなく、流体に含まれる成分の濃度計測を行うことが必要とされる用途がある。 There are applications where it is necessary to measure the concentration of components contained in a fluid without being affected by turbulence in the fluid flowing through a channel.

従来、流体の成分を測定する計測装置として、超音波流量計の流量計測部を流れる流体をサンプリングする成分計測部を流量計測部に併設したものが知られている(例えば、特許文献1参照)。 Conventionally, a known measuring device for measuring the components of a fluid is one in which a component measuring section that samples the fluid flowing through the flow measuring section of an ultrasonic flowmeter is provided in addition to the flow measuring section (see, for example, Patent Document 1).

図6は、特許文献1に記載された超音波流量計の一部分の断面図を示したものである。 Figure 6 shows a cross-sectional view of a portion of the ultrasonic flowmeter described in Patent Document 1.

この流量計では、計測流路101は仕切板102で多層に分割して多層流路103を形成している。この多層流路103部に流体の成分を計測する副流路104を併設している。そして、多層流路103部の入口側に計測流路101へ突出部105を配置して流路断面を部分的に絞り、エジェクタ効果により多層流路103aの上流側の開口部106から流体を計測流路101に引き込むことで、ガスメータ内の流体を図示していない開口部から副流路104に流入させている。そして、この副流路104において、赤外線により主流中のガス成分を測定するものである。 In this flowmeter, the measurement flow path 101 is divided into multiple layers by partition plates 102 to form a multilayer flow path 103. A sub-flow path 104 for measuring the components of the fluid is also provided in this multilayer flow path 103. A protrusion 105 is placed on the inlet side of the multilayer flow path 103 to the measurement flow path 101 to partially narrow the flow path cross section, and the ejector effect draws the fluid into the measurement flow path 101 from an opening 106 on the upstream side of the multilayer flow path 103a, causing the fluid in the gas meter to flow into the sub-flow path 104 from an opening not shown. Infrared rays are used in this sub-flow path 104 to measure the gas components in the mainstream.

国際公開第2018/185034号International Publication No. 2018/185034

しかしながら、前記従来の構成では、流体の成分を計測する副流路に主流路の流体を誘引するエジェクタ効果を発揮させるためには、流路断面を部分的に絞らねばならず、圧力損失が発生する。しかし、この圧力損失を小さくすると副流路に流入させる十分な吸引力が得られないという課題がある。 However, in the conventional configuration, in order to exert the ejector effect of drawing the fluid in the main flow path into the sub-flow path where the fluid components are measured, the cross section of the flow path must be partially narrowed, resulting in pressure loss. However, there is an issue that reducing this pressure loss does not provide sufficient suction force to cause the fluid to flow into the sub-flow path.

本発明は、前記従来の課題を解決するもので、流体に含まれる成分の濃度等の特性を計測する副流路に、安定した流れを供給し、主流路での圧力損失が少ない構成の計測装置を提供することを目的とするものである。 The present invention aims to solve the above-mentioned problems of the conventional technology by providing a measuring device that supplies a stable flow to a secondary flow path that measures characteristics such as the concentration of components contained in a fluid, and has a configuration that reduces pressure loss in the main flow path.

前記従来の課題を解決するために、本発明の物理量計測装置は、被計測流体が流れる矩形断面の主流路の長辺を外方向に後退させて形成した第1の後退壁と、この第1の後退壁の上流側に設けた上流開口部と、第1の後退壁の下流側に設けた下流開口部と、第1の後退壁の外方向に設けた上流開口部と下流開口部とを接続する副流路を備え、第1の後退壁の後退長さは、主流路を流れる流体のコアンダ効果により形成される低圧領域が、下流開口部からの流れを誘引するように構成し、副流路の高さは、主流路の高さよりも小さくし、前記被計測流体が流れる方向と前記高さの方向の双方に直交する方向に沿った、前記副流路の幅は、前記主流路の幅よりも小さくすることで、副流路に安定した流れを供給し副流路での計測精度を向上できる。また主流路での圧力損失を低減でき、さらに主流路での流れの乱れを低減できる。 In order to solve the above-mentioned problems, the physical quantity measuring device of the present invention includes a first receding wall formed by receding the long side of a main flow passage having a rectangular cross section in an outward direction, an upstream opening provided on the upstream side of the first receding wall, a downstream opening provided on the downstream side of the first receding wall, and a sub-flow passage connecting the upstream opening and the downstream opening provided on the outward side of the first receding wall, the receding length of the first receding wall is configured so that a low pressure region formed by the Coanda effect of the fluid flowing in the main flow passage attracts a flow from the downstream opening, the height of the sub-flow passage is smaller than the height of the main flow passage , and the width of the sub-flow passage along a direction perpendicular to both the direction of the flow of the fluid to be measured and the direction of the height is smaller than the width of the main flow passage, thereby supplying a stable flow to the sub-flow passage and improving the measurement accuracy in the sub-flow passage. In addition, the pressure loss in the main flow passage can be reduced, and the turbulence of the flow in the main flow passage can be reduced.

また、第1の後退壁に対向する長辺を主流路の外方向に後退させて第2の後退壁とし、第1の後退壁の後退長さは第2の後退壁の後退長さよりも小さくした構成とすることで、助走部出口の両側の壁を共に後退させることにより流れの偏向が生じ易い状態とし、後退距離が小さい側へのコアンダ効果をより確実に発生させることができる。 In addition, the long side opposite the first receding wall is set back outward from the main flow path to form a second receding wall, and the setback length of the first receding wall is set shorter than the setback length of the second receding wall. By setting back both walls of the inlet section outlet, a state in which flow deflection is more likely to occur can be created, and the Coanda effect can be more reliably generated on the side with the smaller setback distance.

また、第1の後退壁に対向する長辺を主流路の外方向に後退させて第2の後退壁とし、第2の後退壁の上流側には、助走部に設けた助走開口部と第2の後退壁の上流端に設けた開口部とを接続するバイアス流路を備えた構成とすることで、コアンダ効果による自由噴流の第1の後退壁への流れの偏向に加えて、バイアス流路の流れにより自由噴流の第1の後退壁への付着をより強固なものとし、副流路における流れの生成をさらに確実なものとすることができる。 The long side opposite the first receding wall is set back outward from the main flow path to form a second receding wall, and the upstream side of the second receding wall is provided with a bias flow path that connects the approach opening in the approach section with the opening at the upstream end of the second receding wall. In addition to the deflection of the free jet flow toward the first receding wall due to the Coanda effect, the flow in the bias flow path further strengthens the adhesion of the free jet to the first receding wall, and the generation of flow in the secondary flow path can be further ensured.

本発明の物理量計測装置は、矩形断面の主流路の長辺の一部を外方向に後退させて形成した第1の後退壁を備え、この第1の後退壁の後退長さは、主流路を流れる流体のコアンダ効果により形成される低圧領域が下流開口からの流れを誘引するように構成することで、副流路に安定した流れを供給し副流路での計測精度を向上でき、また主流路での圧力損失の低減でき、主流路での流れの乱れを低減できる。 The physical quantity measuring device of the present invention is equipped with a first receding wall formed by receding part of the long side of the main flow passage with a rectangular cross section outward, and the receding length of this first receding wall is configured so that the low pressure area formed by the Coanda effect of the fluid flowing through the main flow passage attracts the flow from the downstream opening, thereby providing a stable flow to the secondary flow passage and improving the measurement accuracy in the secondary flow passage, and also reducing pressure loss in the main flow passage and turbulence in the main flow passage.

本発明の実施の形態1における物理量計測装置の構成断面図FIG. 1 is a cross-sectional view showing a configuration of a physical quantity measuring device according to a first embodiment of the present invention. (a)本発明の実施の形態1における物理量計測装置の平面図、(b)図1のA矢視図1A is a plan view of a physical quantity measuring device according to a first embodiment of the present invention; FIG. 本発明の実施の形態2における物理量計測装置の構成断面図FIG. 11 is a cross-sectional view showing the configuration of a physical quantity measuring device according to a second embodiment of the present invention. 本発明の実施の形態2における図3のA矢視図3 in the second embodiment of the present invention. 本発明の実施の形態3における物理量計測装置の構成断面図FIG. 11 is a cross-sectional view showing the configuration of a physical quantity measuring device according to a third embodiment of the present invention. 従来の成分計測部の構成を示す断面図Cross-sectional view showing the configuration of a conventional component measuring unit.

第1の発明は、被計測流体が流れる矩形断面の主流路と、前記主流路の一部により形成される助走部と、前記助走部より下流において前記矩形断面の主流路の長辺を外方向に後退させて形成した第1の後退壁と、前記第1の後退壁の上流側に設けた上流開口部と、前記第1の後退壁の下流側に設けた下流開口部と、前記第1の後退壁の外方向に設けられ前記上流開口部と前記下流開口部とを接続する副流路と、前記副流路に配置した一対の超音波送受波器と、前記被計測流体の温度を検知する温度センサと、前記一対の前記超音波送受波器からの信号と前記温度センサからの信号を受けて流体の成分濃度を判別する信号処理部を備え、前記第1の後退壁の後退長さは、前記主流路を流れる流体のコアンダ効果により形成される低圧領域が、前記下流開口からの流れを誘引するように構成することで、副流路に安定した流れを供給し副流路での計測精度を向上でき、主流路での圧力損失の低減でき、主流路での流れの乱れを低減できる。 The first invention includes a main flow path with a rectangular cross section through which a fluid to be measured flows, an approach section formed by a part of the main flow path, a first receding wall formed by receding the long side of the main flow path with a rectangular cross section outward downstream of the approach section, an upstream opening provided on the upstream side of the first receding wall, a downstream opening provided on the downstream side of the first receding wall, a secondary flow path provided on the outer side of the first receding wall and connecting the upstream opening and the downstream opening, a pair of ultrasonic transmitter-receivers arranged in the secondary flow path, a temperature sensor for detecting the temperature of the fluid to be measured, and a signal processing unit for receiving signals from the pair of ultrasonic transmitter-receivers and signals from the temperature sensor to determine the component concentration of the fluid, and the receding length of the first receding wall is configured so that a low-pressure region formed by the Coanda effect of the fluid flowing through the main flow path attracts a flow from the downstream opening, thereby providing a stable flow to the secondary flow path, improving the measurement accuracy in the secondary flow path, reducing pressure loss in the main flow path, and reducing flow turbulence in the main flow path.

第2の発明は、前記第1の後退壁に対向する長辺を前記主流路の外方向に後退させて第2の後退壁を形成し、前記第1の後退壁の後退長さは前記第2の後退壁の後退長さよりも小さくしたことを特徴とすることで、助走部出口の両側の壁を共に後退させることにより流れの偏向が生じ易い状態とし、後退距離が小さい側へのコアンダ効果をより確実に発生させることができる。 The second invention is characterized in that the long side opposite the first receding wall is set back outward from the main flow path to form a second receding wall, and the setback length of the first receding wall is set to be smaller than the setback length of the second receding wall. By setting back both walls of the inlet section outlet, a state in which flow deflection is likely to occur can be created, and the Coanda effect can be more reliably generated on the side with the smaller setback distance.

第3の発明は、前記第1の後退壁に対向する長辺を前記主流路の外方向に後退させて第2の後退壁を形成し、前記第2の後退壁の上流側には、前記助走部に設けた助走開口部と前記第2の後退壁の上流端に設けた開口部とを接続するバイアス流路を備えたことを特徴
とすることで、コアンダ効果による自由噴流の第1の後退壁への流れの偏向に加えて、バイアス流路の流れにより自由噴流の第1の後退壁への付着をより強固なものとし、副流路における流れの生成をさらに確実なものとすることができる。
The third invention is characterized in that a second retreat wall is formed by receding the long side opposite to the first retreat wall outwardly of the main passage, and a bias passage is provided on the upstream side of the second retreat wall, connecting an inlet opening provided in the inlet section and an opening provided at the upstream end of the second retreat wall.In this way, in addition to deflecting the flow of the free jet towards the first retreat wall due to the Coanda effect, the flow of the bias passage can further strengthen the attachment of the free jet to the first retreat wall, and the generation of a flow in the secondary passage can be further ensured.

以下、本発明の実施の形態について、図面を参照しながら説明する。但し、必要以上に詳細な説明は省略する場合がある。例えば、既によく知られた事項の詳細説明、または、実質的に同一の構成に対する重複説明を省略する場合がある。 Below, an embodiment of the present invention will be described with reference to the drawings. However, more detailed explanation than necessary may be omitted. For example, detailed explanation of already well-known matters or duplicate explanation of substantially the same configuration may be omitted.

なお、添付図面および以下の説明は、当業者が本開示を十分に理解するために提供されるのであって、これらにより特許請求の範囲に記載の主題を限定することを意図していない。 The accompanying drawings and the following description are provided to enable those skilled in the art to fully understand the present disclosure, and are not intended to limit the subject matter described in the claims.

(実施の形態1)
実施の形態1について、図1~図2を用いて説明する。
(Embodiment 1)
The first embodiment will be described with reference to FIGS. 1 and 2. FIG.

図1は本発明の実施の形態1における物理量計測装置の構成断面図であり、図2(a)は本発明の実施の形態1における図1のG方向から見た平面図、図2(b)は、図1のA方向から見たA矢視図である。 Figure 1 is a cross-sectional view of the configuration of a physical quantity measuring device in embodiment 1 of the present invention, Figure 2(a) is a plan view of embodiment 1 of the present invention as seen from direction G in Figure 1, and Figure 2(b) is a view as seen from direction A in Figure 1.

図1、図2において、物理量計測装置20は、主流路部21と副流路部22と信号処理部12から構成され、主流路部21の内部には、被計測流体が流れる主流路1が形成され、副流路部22の内部には主流路1に連通する副流路8が形成されている。 In Figures 1 and 2, the physical quantity measuring device 20 is composed of a main flow path section 21, a sub-flow path section 22, and a signal processing section 12. Inside the main flow path section 21, a main flow path 1 through which the fluid to be measured flows is formed, and inside the sub-flow path section 22, a sub-flow path 8 that communicates with the main flow path 1 is formed.

被計測流体が流れる主流路1は、その断面が長辺1aを幅W、短辺1bを高さHで示すアスペクト比が大きく二次元流れを実現する矩形断面の流路であり、主流路1は入口2および出口3を備える。主流路1の入口2側には主流路1の一部により形成される助走部4を設け、この助走部4の下流側には長辺1aの一部を主流路1の外方向に後退長さDとして後退させて形成した第1の後退壁5を配置している。この第1の後退壁5の上流側には上流開口部6を設けるとともに下流側には下流開口部7を設けている。 The main flow channel 1 through which the fluid to be measured flows is a rectangular flow channel with a large aspect ratio, with the long side 1a being the width W and the short side 1b being the height H, realizing a two-dimensional flow, and the main flow channel 1 has an inlet 2 and an outlet 3. An approach section 4 formed by a part of the main flow channel 1 is provided on the inlet 2 side of the main flow channel 1, and a first receding wall 5 formed by receding a part of the long side 1a outwardly of the main flow channel 1 by a receding length D is disposed downstream of this approach section 4. An upstream opening 6 is provided upstream of this first receding wall 5, and a downstream opening 7 is provided downstream of it.

第1の後退壁5の主流路1に対して外方には、上流開口部6と下流開口部7とを接続する長さLの副流路8を設けている。この副流路8には流れ方向に対向配置した一対の超音波送受波器9、10と流体の温度を検知する温度センサ11を配置している。 Outside the main flow passage 1 of the first receding wall 5, a sub-flow passage 8 of length L is provided, connecting the upstream opening 6 and the downstream opening 7. In this sub-flow passage 8, a pair of ultrasonic transmitters 9 and 10 are arranged opposite each other in the flow direction, and a temperature sensor 11 is arranged to detect the temperature of the fluid.

この一対の超音波送受波器9、10と温度センサ11は信号処理部12と電気的に接続され、この信号処理部12はこの一対の超音波送受波器9、10からの信号と温度センサ11からの信号を受けて被計測流体の成分濃度を計測する。 The pair of ultrasonic transmitters and receivers 9, 10 and the temperature sensor 11 are electrically connected to a signal processing unit 12, which receives signals from the pair of ultrasonic transmitters and receivers 9, 10 and the temperature sensor 11 to measure the component concentrations of the fluid being measured.

助走部4に対する第1の後退壁5の後退長さDは、主流路1を流れる流体のコアンダ効果により形成される低圧領域Bが、下流開口部7からの流れを誘引するように設定して構成している。また、下流開口部7には流れ方向の上流側に主流路1の内壁に沿って延伸させた流入促進部13を配置し、主流路1から副流路8へ流体が流入し易くしている。なお、副流路8の高さhは、主流路1の高さHよりも小さくして(h<H)、主流路1の流れよりも、副流路8の乱れが小さくなるようにしている。また、副流路8や流入促進部13には流体の流れが滑らかになるように、曲がり部等にはコーナR(丸み付け)を行っている。 The setback length D of the first setback wall 5 relative to the approach section 4 is set so that the low pressure region B formed by the Coanda effect of the fluid flowing through the main channel 1 attracts the flow from the downstream opening 7. In addition, an inflow promotion section 13 extending along the inner wall of the main channel 1 is arranged on the upstream side of the flow direction of the downstream opening 7, making it easier for the fluid to flow from the main channel 1 to the secondary channel 8. The height h of the secondary channel 8 is smaller than the height H of the main channel 1 (h<H), so that the turbulence in the secondary channel 8 is smaller than that in the main channel 1. In addition, corners of the secondary channel 8 and the inflow promotion section 13 are rounded to smooth the flow of the fluid.

次に、本発明の物理量計測装置20の動作について説明する。 Next, the operation of the physical quantity measuring device 20 of the present invention will be described.

主流路1を流れる被計測流体は、入口2から図1の白抜き矢印で示すように流入し、助
走部4からの流れF1は、断面が急拡大する第1の後退壁5部に来ると、低圧の渦領域である低圧領域Bを形成する。この低圧領域Bの負圧により、流れF1は第1の後退壁5の壁面に再付着する流れをコアンダ効果により形成する。このとき低圧になった低圧領域Bは上流開口部6を介して副流路8の被計測流体を誘引する。一方、第1の後退壁5の壁面に再付着した流れF2は下流開口部7に達すると、下流開口部7に流入し、副流路8に安定した穏やかな流れを供給する。
The fluid to be measured flowing through the main flow passage 1 flows in from the inlet 2 as shown by the white arrow in Fig. 1, and when the flow F1 from the inlet 4 reaches the first receding wall 5 where the cross section suddenly expands, it forms a low-pressure region B, which is a low-pressure vortex region. Due to the negative pressure of this low-pressure region B, the flow F1 forms a flow that reattaches to the wall surface of the first receding wall 5 due to the Coanda effect. At this time, the low-pressure region B, which has become low pressure, attracts the fluid to be measured in the sub-flow passage 8 through the upstream opening 6. On the other hand, when the flow F2 that reattaches to the wall surface of the first receding wall 5 reaches the downstream opening 7, it flows into the downstream opening 7 and supplies a stable and gentle flow to the sub-flow passage 8.

副流路8では、その高さhは、主流路1の高さHよりも小さく設定されているため、副流路8における流れの乱れは、主流路1の流れの乱れよりも小さくなる。また、上流開口部6、下流開口部7および流入促進部13を含めた曲がり部などにはコーナR(丸み付け)を付与するとともに断面積の急変を避けるように構成している。このため、副流路8での流れF3は、流れが一層滑らかになるようにされている。 The height h of the secondary flow passage 8 is set smaller than the height H of the main flow passage 1, so the turbulence of the flow in the secondary flow passage 8 is smaller than that in the main flow passage 1. In addition, corners R (rounding) are given to bends including the upstream opening 6, downstream opening 7, and inflow promotion section 13, and the like, and a sudden change in cross-sectional area is avoided. As a result, the flow F3 in the secondary flow passage 8 is made to flow more smoothly.

従って、副流路8において、主流路1での流体と副流路8での流体が滞留すること無く流動するという流体成分の濃度計測に必要な条件を満たしているため、副流路8において一対の超音波送受波器9、10を用いて音速を計測し、温度センサ11からの流体の温度と合わせて、公知の方法で、流体に含まれる成分濃度を計測することができる。 Therefore, the sub-channel 8 satisfies the condition necessary for measuring the concentration of fluid components, that is, the fluid in the main channel 1 and the fluid in the sub-channel 8 flow without stagnation. Therefore, the sound speed is measured in the sub-channel 8 using a pair of ultrasonic transmitters 9 and 10, and the concentration of components contained in the fluid can be measured by a known method, together with the fluid temperature from the temperature sensor 11.

このように副流路8では、主流路1の流体が滞留すること無く流入し、主流路1の流体と濃度等も均一で穏やかで、乱れの少ない安定した流れを実現するため、計測の信頼性や計測精度を高めることができる。 In this way, the fluid from the main flow path 1 flows into the sub-flow path 8 without stagnation, and the concentration of the fluid in the main flow path 1 is uniform and gentle, achieving a stable flow with little turbulence, thereby improving the reliability and accuracy of measurements.

(実施の形態2)
実施の形態2について、図3~図4を用いて説明する。
図3は本発明の実施の形態2における物理量計測装置の構成断面図であり、図4は本発明の実施の形態2における図3のA方向から見たA矢視図である。なお、実施の形態1と同じ機能のものは同一番号を付して詳細な説明は省略する。
(Embodiment 2)
The second embodiment will be described with reference to FIGS.
Fig. 3 is a cross-sectional view of the configuration of a physical quantity measuring device according to a second embodiment of the present invention, and Fig. 4 is a view taken along the arrow A in Fig. 3 according to the second embodiment of the present invention. Note that components having the same functions as those in the first embodiment are given the same reference numbers and detailed descriptions thereof will be omitted.

図3、図4において、第1の後退壁5を設けた長辺1aと反対側にある対向する長辺1c側にも、長辺1cの一部を主流路1の外方向に後退長さEとして後退させて形成した第2の後退壁14を配置している。ここで、助走部4に対する第1の後退壁5の後退長さDは、第2の後退壁14の後退長さEよりも小さく(D<E)設定して構成している。 In Figures 3 and 4, a second setback wall 14 is also disposed on the opposing long side 1c opposite the long side 1a on which the first setback wall 5 is provided, by setting back a portion of the long side 1c outward from the main flow path 1 by a setback length E. Here, the setback length D of the first setback wall 5 relative to the inlet 4 is set to be smaller than the setback length E of the second setback wall 14 (D<E).

次に、本発明の物理量計測装置30の動作について説明する。
主流路1を流れる被計測流体は、第2の後退壁14側でも第1の後退壁5側と同様に、第2の後退壁14の上流部に低圧の渦領域である低圧領域Gを形成する。
Next, the operation of the physical quantity measuring device 30 of the present invention will be described.
The fluid to be measured flowing through the main flow passage 1 forms a low-pressure region G, which is a low-pressure vortex region, upstream of the second receding wall 14 on the second receding wall 14 side as well as on the first receding wall 5 side.

実施の形態2では、第1の後退壁5および第2の後退壁14により図5における上下方向に断面が急拡大となるため、助走部4の下流端部から流出する流れが自由噴流の状態になり、流れの偏向が生じ易い条件となる。 In the second embodiment, the first receding wall 5 and the second receding wall 14 cause the cross section to expand rapidly in the vertical direction in FIG. 5, so the flow flowing out from the downstream end of the inlet section 4 becomes a free jet, creating conditions that make the flow prone to deflection.

しかし、ここでは第1の後退壁5の後退長さDと第2の後退壁14の後退長さEは異なる大きさであり、第1の後退壁5の後退長さDは第2の後退壁14の後退長さEよりも小さく(D<E)設定されている。このため、低圧の渦領域である低圧領域Bおよび低圧領域Gでの圧力に違いを生じ、第1の後退壁5側の低圧領域Bは第2の後退壁14側の低圧領域Gよりも低い圧力となる。 However, here, the retreat length D of the first retreat wall 5 and the retreat length E of the second retreat wall 14 are different sizes, and the retreat length D of the first retreat wall 5 is set to be smaller than the retreat length E of the second retreat wall 14 (D<E). This causes a difference in pressure in the low pressure region B, which is a low pressure vortex region, and the low pressure region B on the first retreat wall 5 side has a lower pressure than the low pressure region G on the second retreat wall 14 side.

従って、助走部4の下流端部から流出する自由噴流は、後退長さが小さい第1の後退壁5側にコアンダ効果を強く受けて、より一層確実に第1の後退壁5に付着する。 Therefore, the free jet flowing out from the downstream end of the inlet section 4 is more strongly affected by the Coanda effect on the side of the first receding wall 5, which has a smaller retreat length, and adheres to the first receding wall 5 more reliably.

このように低圧領域Bの負圧効果と確実に付着する流れF1を形成することにより、副流路8に安定した穏やかな流れの一層確実な形成がなされる。 In this way, by forming a flow F1 that reliably adheres to the negative pressure effect of the low pressure area B, a stable and gentle flow is more reliably formed in the secondary flow path 8.

このように、助走部4の下流端部の両側の壁を共に後退させることにより流れの偏向が生じ易い状態とし、後退距離が小さい側へのコアンダ効果をより確実に発生させることで、より一層確実に副流路8に穏やかで安定した流れを供給し、流体に含まれる成分濃度を計測する計測精度の向上や計測の信頼性を高めることができる。 In this way, by receding both walls at the downstream end of the inlet section 4, a state is created in which flow deflection is more likely to occur, and the Coanda effect is more reliably generated on the side with the smaller receding distance, which more reliably supplies a gentle and stable flow to the secondary flow path 8, improving the measurement accuracy and reliability of measuring the concentration of components contained in the fluid.

(実施の形態3)
実施の形態3について、図5を用いて説明する。
図5は本発明の実施の形態3における物理量計測装置の構成断面図である。なお、実施の形態1および実施の形態2と同じ機能のものは同一番号を付して詳細な説明は省略する。
(Embodiment 3)
The third embodiment will be described with reference to FIG.
5 is a cross-sectional view of the configuration of a physical quantity measuring device according to a third embodiment of the present invention. Note that components having the same functions as those in the first and second embodiments are given the same reference numbers and detailed descriptions thereof will be omitted.

図5において、実施の形態2の図4に示したものと同様に本実施の形態3においても第1の後退壁5を設けた長辺1a(図示せず)と反対側にある対向する長辺1c(図示せず)側にも、長辺1c(図示せず)の一部を主流路1の外方向に後退長さKとして後退させて形成した第2の後退壁14を配置している。ここでは、助走部4に対する第2の後退壁14の後退長さKは、第1の後退壁5の後退長さDとほぼ同等(K≒D)に設定して構成している。 In FIG. 5, similar to that shown in FIG. 4 of the second embodiment, in the third embodiment, a second receding wall 14 is disposed on the opposing long side 1c (not shown) opposite the long side 1a (not shown) on which the first receding wall 5 is provided, by receding a portion of the long side 1c (not shown) outwardly of the main flow path 1 by a receding length K. Here, the receding length K of the second receding wall 14 relative to the inlet 4 is set to be approximately equal to the receding length D of the first receding wall 5 (K ≒ D).

この第2の後退壁14の上流側の助走部4には助走開口部15を設け、さらに第2の後退壁14の上流端に開口部16を設けるとともに、この助走開口部15と開口部16とをバイアス流路17で接続している。 An approach opening 15 is provided in the approach section 4 upstream of the second receding wall 14, and an opening 16 is provided at the upstream end of the second receding wall 14, and the approach opening 15 and opening 16 are connected by a bias flow path 17.

次に、本発明の物理量計測装置40の動作について説明する。 Next, the operation of the physical quantity measuring device 40 of the present invention will be described.

主流路1を流れる被計測流体は、第1の後退壁5および第2の後退壁14により図5における上下方向に断面が急拡大となるため、助走部4の下流端部から流出する流れは自由噴流の状態になり、流れの偏向が生じ易い条件となる。 The measured fluid flowing through the main flow path 1 has a cross section that expands rapidly in the vertical direction in FIG. 5 due to the first receding wall 5 and the second receding wall 14, so the flow flowing out from the downstream end of the inlet section 4 becomes a free jet, creating conditions that make it easy for flow deflection to occur.

実施の形態3では、第2の後退壁14の上流端部において、助走開口部15から流入しバイアス流路17を流れるバイアス流F5が開口部16から流入する。 In the third embodiment, at the upstream end of the second receding wall 14, the bias flow F5 that flows in from the inlet opening 15 and flows through the bias flow path 17 flows in from the opening 16.

助走部4より流出する自由噴流は、第1の後退壁5にコアンダ効果による自由噴流の偏向だけでなく、第2の後退壁14の上流端から流入するバイアス流F5の流れが図5における上方に自由噴流を押し上げるように作用するため、自由噴流の第1の後退壁5への付着がより強固になされ、副流路8における流れの生成をさらに確実なものとすることができる。 The free jet flowing out from the inlet section 4 is not only deflected by the Coanda effect on the first receding wall 5, but also the bias flow F5 flowing in from the upstream end of the second receding wall 14 acts to push the free jet upward in FIG. 5, so that the free jet adheres more firmly to the first receding wall 5, further ensuring the generation of a flow in the secondary flow passage 8.

このように、助走部4の下流端部の両側の壁を共に後退させることにより流れの偏向が生じ易い状態とし、コアンダ効果による自由噴流の第1の後退壁5への流れの偏向に加えて、バイアス流路17の流れにより自由噴流の第1の後退壁5への付着をより強固なものとし、副流路8における流れの生成をさらに確実なものとすることができる。 In this way, by receding both walls at the downstream end of the inlet section 4, a state is created in which flow deflection is more likely to occur. In addition to the flow deflection of the free jet toward the first receding wall 5 due to the Coanda effect, the flow of the bias flow passage 17 strengthens the adhesion of the free jet to the first receding wall 5, further ensuring the generation of flow in the secondary flow passage 8.

以上、本発明の実施の形態において、副流路8の幅(図1、図3、図5における奥行き方向)は主流路1の幅W方向の長辺1aの幅の一部で説明したが、幅W方向の全域であっても良い。また、流体の成分を計測する物理量計測装置として説明したが、主流路1での圧力損失の低減だけでなく、主流路1での流れの乱れを低減し安定化できるので、主流路1の上流側あるいは下流側に流量計測部を直列に配置した流量計、あるいは副流路8を有する主流路1に流量計測部を並列配置した流量計として展開できるのは云うまでもない。 In the above embodiments of the present invention, the width of the sub-channel 8 (depth direction in Figs. 1, 3, and 5) has been described as a part of the width of the long side 1a in the width W direction of the main channel 1, but it may be the entire width W direction. Also, although it has been described as a physical quantity measuring device that measures the components of a fluid, it goes without saying that it can be deployed as a flowmeter in which a flow rate measuring unit is arranged in series on the upstream or downstream side of the main channel 1, or as a flowmeter in which a flow rate measuring unit is arranged in parallel to the main channel 1 having the sub-channel 8, since it can reduce not only the pressure loss in the main channel 1 but also reduce and stabilize the turbulence of the flow in the main channel 1.

以上のように、本発明の物理量計測装置は、副流路に安定した流れを供給し主流路での圧力損失が少ない構成の計測装置を提供できるもので、主流路での流れの安定化も可能となるので、流体の成分の計測装置だけで無く、流量計測部を併設して計測精度および汎用性の高い流量計を実現できる。 As described above, the physical quantity measuring device of the present invention can provide a measuring device that supplies a stable flow to the secondary flow path and has a configuration with little pressure loss in the main flow path, and it is also possible to stabilize the flow in the main flow path, so that it is not only a measuring device for the components of the fluid, but also a flow meter with high measurement accuracy and versatility can be realized by incorporating a flow rate measuring unit.

1 主流路
2 入口
3 出口
4 助走部
5 第1の後退壁
6 上流開口部
7 下流開口部
8 副流路
9、10 超音波送受波器
11 温度センサ
12 信号処理部
13 流入促進部
14 第2の後退壁
15 助走開口部
16 開口部
17 バイアス流路
20、30、40 物理量計測装置
REFERENCE SIGNS LIST 1 Main flow path 2 Inlet 3 Outlet 4 Approach section 5 First receding wall 6 Upstream opening 7 Downstream opening 8 Sub-flow path 9, 10 Ultrasonic transmitter/receiver 11 Temperature sensor 12 Signal processing section 13 Inflow promotion section 14 Second receding wall 15 Approach opening 16 Opening 17 Bias flow path 20, 30, 40 Physical quantity measuring device

Claims (3)

被計測流体が流れる矩形断面の主流路と、
前記主流路の一部により形成される助走部と、
前記助走部より下流において前記矩形断面の前記主流路の長辺を外方向に後退させて形成した第1の後退壁と、
前記第1の後退壁の上流側に設けた上流開口部と、
前記第1の後退壁の下流側に設けた下流開口部と、
前記第1の後退壁の外方向に設けられ前記上流開口部と前記下流開口部とを接続する副流路と、
前記副流路に配置した一対の超音波送受波器と、
前記被計測流体の温度を検知する温度センサと、
前記一対の前記超音波送受波器からの信号と前記温度センサからの信号を受けて流体の成分濃度を判別する信号処理部と、を備え、
前記第1の後退壁の後退長さは、前記主流路を流れる流体のコアンダ効果により形成される低圧領域が、前記下流開口部からの流れを誘引するように構成し、
前記副流路の高さは、前記主流路の高さよりも小さくし
前記被計測流体が流れる方向と前記高さの方向の双方に直交する方向に沿った、前記副流路の幅は、前記主流路の幅よりも小さくした物理量計測装置。
a main flow path having a rectangular cross section through which a fluid to be measured flows;
an inlet portion formed by a part of the main flow path;
a first receding wall formed by receding a long side of the main flow passage having a rectangular cross section outward downstream of the inlet portion;
an upstream opening provided on the upstream side of the first receding wall;
a downstream opening provided on a downstream side of the first receding wall;
a sub-flow passage provided outside the first receding wall and connecting the upstream opening and the downstream opening;
A pair of ultrasonic transducers disposed in the sub-channel;
A temperature sensor that detects the temperature of the fluid to be measured;
a signal processing unit that receives signals from the pair of ultrasonic transmitters and receivers and a signal from the temperature sensor and determines the component concentration of the fluid,
The recessed length of the first recessed wall is configured so that a low pressure region formed by the Coanda effect of the fluid flowing through the main flow path induces a flow from the downstream opening,
The height of the sub-channel is smaller than the height of the main channel ,
A physical quantity measuring device , wherein a width of the sub-channel along a direction perpendicular to both the direction in which the fluid to be measured flows and the height direction is smaller than a width of the main channel .
被計測流体が流れる矩形断面の主流路と、
前記主流路の一部により形成される助走部と、
前記助走部より下流において前記矩形断面の前記主流路の長辺を外方向に後退させて形成した第1の後退壁と、
前記第1の後退壁の上流側に設けた上流開口部と、
前記第1の後退壁の下流側に設けた下流開口部と、
前記第1の後退壁の外方向に設けられ前記上流開口部と前記下流開口部とを接続する副流路と、
前記副流路に配置した一対の超音波送受波器と、
前記被計測流体の温度を検知する温度センサと、
前記一対の前記超音波送受波器からの信号と前記温度センサからの信号を受けて流体の
成分濃度を判別する信号処理部と、を備え、
前記第1の後退壁の後退長さは、前記主流路を流れる流体のコアンダ効果により形成される低圧領域が、前記下流開口部からの流れを誘引するように構成し、
前記第1の後退壁に対向する長辺を前記主流路の外方向に後退させて第2の後退壁を形成し、前記第1の後退壁の後退長さは前記第2の後退壁の後退長さよりも小さくした物理量計測装置。
a main flow path having a rectangular cross section through which a fluid to be measured flows;
an inlet portion formed by a part of the main flow path;
a first receding wall formed by receding a long side of the main flow passage having a rectangular cross section outward downstream of the inlet portion;
an upstream opening provided on the upstream side of the first receding wall;
a downstream opening provided on a downstream side of the first receding wall;
a sub-flow passage provided outside the first receding wall and connecting the upstream opening and the downstream opening;
A pair of ultrasonic transducers disposed in the sub-channel;
A temperature sensor that detects the temperature of the fluid to be measured;
a signal processing unit that receives signals from the pair of ultrasonic transmitters and receivers and a signal from the temperature sensor and determines the component concentration of the fluid,
The recessed length of the first recessed wall is configured so that a low pressure region formed by the Coanda effect of the fluid flowing through the main flow path induces a flow from the downstream opening,
a second receding wall is formed by receding a long side opposite to the first receding wall outwardly of the main flow path, and a receding length of the first receding wall is made smaller than a receding length of the second receding wall.
被計測流体が流れる矩形断面の主流路と、
前記主流路の一部により形成される助走部と、
前記助走部より下流において前記矩形断面の前記主流路の長辺を外方向に後退させて形成した第1の後退壁と、
前記第1の後退壁の上流側に設けた上流開口部と、
前記第1の後退壁の下流側に設けた下流開口部と、
前記第1の後退壁の外方向に設けられ前記上流開口部と前記下流開口部とを接続する副流路と、
前記副流路に配置した一対の超音波送受波器と、
前記被計測流体の温度を検知する温度センサと、
前記一対の前記超音波送受波器からの信号と前記温度センサからの信号を受けて流体の成分濃度を判別する信号処理部と、を備え、
前記第1の後退壁の後退長さは、前記主流路を流れる流体のコアンダ効果により形成される低圧領域が、前記下流開口部からの流れを誘引するように構成し、
前記第1の後退壁に対向する長辺を前記主流路の外方向に後退させて第2の後退壁を形成し、前記第2の後退壁の上流側には、前記助走部に設けた助走開口部と前記第2の後退壁の上流端に設けた開口部とを接続するバイアス流路を備えた物理量計測装置。
a main flow path having a rectangular cross section through which a fluid to be measured flows;
an inlet portion formed by a part of the main flow path;
a first receding wall formed by receding a long side of the main flow passage having a rectangular cross section outward downstream of the inlet portion;
an upstream opening provided on the upstream side of the first receding wall;
a downstream opening provided on a downstream side of the first receding wall;
a sub-flow passage provided outside the first receding wall and connecting the upstream opening and the downstream opening;
A pair of ultrasonic transducers disposed in the sub-channel;
A temperature sensor that detects the temperature of the fluid to be measured;
a signal processing unit that receives signals from the pair of ultrasonic transmitters and receivers and a signal from the temperature sensor and determines the component concentration of the fluid,
The recessed length of the first recessed wall is configured so that a low pressure region formed by the Coanda effect of the fluid flowing through the main flow path induces a flow from the downstream opening,
a second receding wall is formed by receding a long side opposite to the first receding wall outwardly of the main flow path, and a bias flow path is provided on the upstream side of the second receding wall, connecting an approach opening provided in the approach section and an opening provided at the upstream end of the second receding wall.
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Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2014071109A (en) 2012-09-28 2014-04-21 Hokushin Electronics:Kk Ultrasonic gas concentration meter
US20140238364A1 (en) 2013-02-28 2014-08-28 Bendix Commercial Vehicle Systems Llc Method to Enhance Gas Recirculation in Turbocharged Diesel Engines
JP2015224870A (en) 2014-05-26 2015-12-14 株式会社ホクシンエレクトロニクス Ultrasonic gas measuring device

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2014071109A (en) 2012-09-28 2014-04-21 Hokushin Electronics:Kk Ultrasonic gas concentration meter
US20140238364A1 (en) 2013-02-28 2014-08-28 Bendix Commercial Vehicle Systems Llc Method to Enhance Gas Recirculation in Turbocharged Diesel Engines
JP2015224870A (en) 2014-05-26 2015-12-14 株式会社ホクシンエレクトロニクス Ultrasonic gas measuring device

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