JPH0321452Y2 - - Google Patents
Info
- Publication number
- JPH0321452Y2 JPH0321452Y2 JP1984183676U JP18367684U JPH0321452Y2 JP H0321452 Y2 JPH0321452 Y2 JP H0321452Y2 JP 1984183676 U JP1984183676 U JP 1984183676U JP 18367684 U JP18367684 U JP 18367684U JP H0321452 Y2 JPH0321452 Y2 JP H0321452Y2
- Authority
- JP
- Japan
- Prior art keywords
- upstream
- karman vortex
- rectifying
- downstream
- grating
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 238000011144 upstream manufacturing Methods 0.000 claims description 23
- 239000012530 fluid Substances 0.000 claims description 5
- 238000005259 measurement Methods 0.000 description 6
- 238000010586 diagram Methods 0.000 description 5
- 230000000694 effects Effects 0.000 description 3
- 230000007423 decrease Effects 0.000 description 2
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 239000011888 foil Substances 0.000 description 1
Description
【考案の詳細な説明】
〔考案の属する技術分野〕
本考案は、管路内を流れる流体、例えば自動車
等のエンジンの吸入空気量を測定するために、流
体中に挿入されたカルマン渦発生体により発生す
るカルマン渦列を検出して流量を測定するカルマ
ン渦流量計に関する。[Detailed description of the invention] [Technical field to which the invention pertains] The present invention is a Karman vortex generator inserted into a fluid flowing in a pipe, for example, in order to measure the intake air amount of an engine such as an automobile. This invention relates to a Karman vortex flow meter that measures flow rate by detecting the Karman vortex street generated by.
〔従来技術とその問題点〕
この種のエンジンの吸入空気量を測定する渦流
量計として例えば特公昭56−34046号公報が公知
である。この公報に開示された渦流量計において
は、管路入口の絞り管の上流側に1個の整流格子
を取付けた構成が採用されている。このような構
成の渦流量計について実験を行つたところ、整流
格子による整流効果により、高速域における直線
性に比較して、低速域における直線性が低下する
ことが明らかになつた。従つて、低速域の直線性
の向上による測定精度の改善が要望されていた。[Prior art and its problems] A vortex flowmeter for measuring the intake air amount of this type of engine is known, for example, in Japanese Patent Publication No. 34046/1983. The vortex flowmeter disclosed in this publication employs a configuration in which one rectifying grid is attached to the upstream side of the throttle tube at the entrance of the conduit. When conducting experiments on a vortex flow meter with such a configuration, it was found that due to the rectifying effect of the rectifying grid, the linearity in the low speed range is lower than that in the high speed range. Therefore, it has been desired to improve measurement accuracy by improving linearity in the low speed range.
本考案は、上述の点に鑑み、従来技術の問題点
を有効に解決し、その構成が簡単で、しかも低流
速域において測定精度の直線性が向上するカルマ
ン渦流量計を提供することを目的とする。
In view of the above-mentioned points, the purpose of the present invention is to provide a Karman vortex flowmeter that effectively solves the problems of the conventional technology, has a simple configuration, and improves the linearity of measurement accuracy in the low flow velocity region. shall be.
このような目的を達成するために、本考案は、
被測定流体が流れる管路内に挿入された渦発生体
により発生するカルマン渦列を検出して流量を測
定するカルマン渦流量計において、前記管路の過
発生体挿入位置よりも上流側に絞り部を設けると
ともに、この絞り部の直前および直後に、それぞ
れ、上流側整流格子および下流側整流格子を配設
し、かつ、該上流側整流格子の目を下流側整流格
子の目よりも細かくする。
In order to achieve this purpose, the present invention
In a Karman vortex flowmeter that measures the flow rate by detecting the Karman vortex street generated by a vortex generator inserted into a pipe through which a fluid to be measured flows, a constrictor is installed upstream of the position where the excess generator is inserted in the pipe. an upstream rectifying grating and a downstream rectifying grating are provided immediately before and after the constricted part, respectively, and the mesh of the upstream rectifying grating is finer than that of the downstream rectifying grating. .
次に、本考案の一実施例を図面に基づき、詳細
に説明する。
Next, one embodiment of the present invention will be described in detail based on the drawings.
第1図は本考案の一実施例の概略構成図を示
し、Aはその正面断面図、Bはその側面図であ
る。図においてカルマン渦流量計1は、主として
管路2、管路2の内部に挿入されたカルマン渦発
生体3、カルマン渦検出部4および上流側ならび
に下流側整流格子5,6から構成される。管路2
は、本実施例では角型に形成される。カルマン渦
発生体3は、断面二等辺三角形状に形成された上
流側柱状体7および断面台形に形成された下流側
柱状体8とからなる。また、カルマン渦検出部4
は、カルマン渦発生体3により流体の流れに発生
したカルマン渦列を検出して流量を測定する。 FIG. 1 shows a schematic diagram of an embodiment of the present invention, in which A is a front sectional view and B is a side view. In the figure, the Karman vortex flowmeter 1 mainly includes a pipe line 2, a Karman vortex generator 3 inserted into the pipe line 2, a Karman vortex detector 4, and upstream and downstream rectifying gratings 5, 6. Conduit 2
is formed into a square shape in this embodiment. The Karman vortex generating body 3 includes an upstream columnar body 7 having an isosceles triangular cross section and a downstream columnar body 8 having a trapezoidal cross section. In addition, the Karman vortex detection unit 4
The flow rate is measured by detecting the Karman vortex street generated in the fluid flow by the Karman vortex generator 3.
ところで、上流側整流格子5は、その外径が大
きく、カルマン渦発生体3の上流側に設置された
絞り管9の大口径側の直前に配置される。また、
下流側整流格子6は、その外径が小さく、絞り管
9の小口径側直後に配置される。このような上流
側および下流側整流格子5,6は、それぞれ厚さ
が約20μmないし50μm程度の薄いアルミニウム箔
から形成された多数のハニカム状構造体からな
る。この上流側および下流側整流格子5,6のハ
ニカム状構造体は、本実施例では上流側整流格子
5がメツシユを約1/8吋程度に形成され、下流側
整流格子6がメツシユを約1/4吋程度に形成され、
従つて上流側整流格子5が下流側整流格子6より
もメツシユを細かく形成されている。なお、10
は流体温度を検出する温度検出器である。 Incidentally, the upstream rectifying grid 5 has a large outer diameter and is disposed immediately in front of the large diameter side of the throttle tube 9 installed upstream of the Karman vortex generator 3. Also,
The downstream rectifying grid 6 has a small outer diameter and is disposed immediately after the small diameter side of the throttle tube 9. The upstream and downstream rectifying gratings 5 and 6 each consist of a large number of honeycomb-like structures made of thin aluminum foil with a thickness of approximately 20 μm to 50 μm. In this embodiment, the upstream and downstream rectifying gratings 5 and 6 have a honeycomb structure in which the upstream rectifying grating 5 has a mesh size of approximately 1/8 inch, and the downstream rectifying grating 6 has a mesh size of approximately 1/8 inch. Formed to about /4 inch,
Therefore, the upstream rectifying grid 5 has a finer mesh than the downstream rectifying grid 6. In addition, 10
is a temperature detector that detects fluid temperature.
第2図は流速V(1m/secないし100msecの範
囲)−ストローハル数st特性図である。この第2
図において、特性線Aは本考案の一実施例の実験
結果を示し、直線性が約±2%程度となつてい
る。これに対して、特性線Bは従来の整流格子が
1段の場合の実験結果を示す。この特性線Bは本
実施例の特性線Aに比較して低流域の直線性が低
下するために、全体としてその直線性が約±3.7
%程度となつている。この実験結果から明らかな
ように、本考案によれば、上流側および下流側整
流格子5,6を絞り管9の直前および直後に配置
し、しかも上流側整流格子5のメツシユを下流側
整流格子6のメツシユより小さくしたことによ
り、その測定精度が大幅に向上される。 FIG. 2 is a characteristic diagram of flow velocity V (in the range of 1 m/sec to 100 msec) versus Strouhal number st. This second
In the figure, characteristic line A shows the experimental results of one embodiment of the present invention, and the linearity is about ±2%. On the other hand, characteristic line B shows the experimental results when the conventional rectifying grid has one stage. This characteristic line B has a lower linearity in the low region than the characteristic line A of this embodiment, so its linearity as a whole is about ±3.7.
It is about %. As is clear from the experimental results, according to the present invention, the upstream and downstream rectifying gratings 5 and 6 are arranged immediately before and after the throttle pipe 9, and the mesh of the upstream rectifying grating 5 is replaced by the mesh of the downstream rectifying grating. By making the mesh smaller than 6, the measurement accuracy is greatly improved.
なお、下流側整流格子6のメツシユを上流側整
流格子5のメツシユよりも細かくすると、低速域
ではカルマン渦列の発生が減少し、測定範囲が減
少するという傾向を有するが、本考案の如く、下
流側整流格子6のメツシユを上流側整流格子5の
メツシユより荒くすることにより、管路1の全体
に細かい乱れが発生し、カルマン渦列の発生を容
易にするものと考える。 Note that if the mesh of the downstream rectifying grating 6 is made finer than that of the upstream rectifying grating 5, there is a tendency that the generation of Karman vortex street decreases in the low speed region and the measurement range decreases, but as in the present invention, It is believed that by making the mesh of the downstream rectifying grid 6 rougher than that of the upstream rectifying grid 5, fine turbulence is generated throughout the pipe line 1, facilitating the generation of the Karman vortex street.
以上に説明するように本考案によれば、管路の
入口に設けられた絞り部9の上流側に上流側整流
格子5および下流側に下流側整流格子6がそれぞ
れ配置され、この上流側整流格子を、下流側整流
格子よりも目を細かく形成することにより、簡単
な構成によつて、低速域における直線性が低下す
るという従来技術の問題点が有効に解決され、そ
れゆえに低速域における直線性が改善され、測定
精度が向上する、測定範囲を広くすることができ
る等の効果が奏される。
As described above, according to the present invention, the upstream rectifying grid 5 and the downstream rectifying grid 6 are arranged on the upstream side and the downstream side of the throttle part 9 provided at the entrance of the pipe, respectively, and the upstream rectifying By forming the grid with finer mesh than the downstream rectifying grid, the problem of the prior art that the linearity in the low speed range is reduced can be effectively solved with a simple configuration, and therefore the straightness in the low speed range can be improved. Effects such as improved performance, improved measurement accuracy, and wider measurement range can be achieved.
第1図は本考案の一実施例の概略構成図を示
し、同図Aはその正面断面図、同図Bはその側面
断面図、第2図は測定流速範囲における直線性に
ついて説明するための流速−ストローハル数特性
図である。
1:カルマン渦流量計、2:管路、3:カルマ
ン渦発生体、5:上流側整流格子、6:下流側整
流格子、9:絞り管。
Fig. 1 shows a schematic configuration diagram of an embodiment of the present invention, Fig. A is a front sectional view thereof, Fig. B is a side sectional view thereof, and Fig. 2 is a diagram for explaining linearity in the measured flow velocity range. It is a flow velocity-Strohal number characteristic diagram. 1: Karman vortex flow meter, 2: pipe line, 3: Karman vortex generator, 5: upstream rectification grid, 6: downstream rectification grid, 9: throttle tube.
Claims (1)
体により発生するカルマン渦列を検出して流量を
測定するカルマン渦流量計において、前記管路の
過発生体挿入位置よりも上流側に絞り部9を設け
るとともに、この絞り部9の直前および直後に、
それぞれ、上流側整流格子5および下流側整流格
子6を配設し、かつ、該上流側整流格子5の目を
下流側整流格子6の目よりも細かくしてなること
を特徴とするカルマン渦流量計。 In a Karman vortex flowmeter that measures the flow rate by detecting the Karman vortex street generated by a vortex generator inserted into a pipe through which a fluid to be measured flows, a constrictor is installed upstream of the position where the excess generator is inserted in the pipe. A section 9 is provided, and immediately before and after this constriction section 9,
A Karman vortex flow rate characterized in that an upstream rectifying grating 5 and a downstream rectifying grating 6 are provided, and the meshes of the upstream rectifying grating 5 are finer than those of the downstream rectifying grating 6. Total.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1984183676U JPH0321452Y2 (en) | 1984-12-05 | 1984-12-05 |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1984183676U JPH0321452Y2 (en) | 1984-12-05 | 1984-12-05 |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6199014U JPS6199014U (en) | 1986-06-25 |
JPH0321452Y2 true JPH0321452Y2 (en) | 1991-05-10 |
Family
ID=30741173
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1984183676U Expired JPH0321452Y2 (en) | 1984-12-05 | 1984-12-05 |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0321452Y2 (en) |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS50116453U (en) * | 1974-03-05 | 1975-09-22 |
-
1984
- 1984-12-05 JP JP1984183676U patent/JPH0321452Y2/ja not_active Expired
Also Published As
Publication number | Publication date |
---|---|
JPS6199014U (en) | 1986-06-25 |
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