JPH0236093Y2 - - Google Patents

Info

Publication number
JPH0236093Y2
JPH0236093Y2 JP1984181241U JP18124184U JPH0236093Y2 JP H0236093 Y2 JPH0236093 Y2 JP H0236093Y2 JP 1984181241 U JP1984181241 U JP 1984181241U JP 18124184 U JP18124184 U JP 18124184U JP H0236093 Y2 JPH0236093 Y2 JP H0236093Y2
Authority
JP
Japan
Prior art keywords
tube
static pressure
pressure
space
head
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
Application number
JP1984181241U
Other languages
Japanese (ja)
Other versions
JPS6194773U (en
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 filed Critical
Priority to JP1984181241U priority Critical patent/JPH0236093Y2/ja
Publication of JPS6194773U publication Critical patent/JPS6194773U/ja
Application granted granted Critical
Publication of JPH0236093Y2 publication Critical patent/JPH0236093Y2/ja
Expired legal-status Critical Current

Links

Landscapes

  • Measuring Volume Flow (AREA)

Description

【考案の詳細な説明】 〔産業上の利用分野〕 本考案は主として空調用ダクト内の空気の流速
を測定する流速計における静圧測定管の構造に関
する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention mainly relates to the structure of a static pressure measuring tube in a current meter that measures the flow velocity of air in an air conditioning duct.

〔従来の技術〕[Conventional technology]

従来の流速計は通常ピトー管でもつて全圧およ
び静圧を測定してその圧力差でもつて流速を計測
している。このピトー管は二重管で内管の先端は
開口して風上方向に向けられて全圧を測定し、外
管と内管との間に形成される空間は密閉され、か
つ、外管側面に前記空間に連通する静圧測定孔を
穿孔させて静圧を測定するものであつた。
Conventional flowmeters usually measure total pressure and static pressure using a pitot tube, and measure the flow rate based on the pressure difference. This Pitot tube is a double tube, with the tip of the inner tube open and facing upwind to measure the total pressure, and the space formed between the outer tube and the inner tube being sealed, and the outer tube Static pressure was measured by drilling a static pressure measurement hole in the side surface that communicated with the space.

これに対し、特開昭59−3315号公報に示すよう
な流速計構造が提案され、この構造においては、
流体輸送管内に流線に対して垂直またはほぼ垂直
な姿勢に挿入される棒状部材の管内挿入部分に、
総圧を電気信号として検出する第1センサーと、
静圧を電気信号として検出する第2センサーとを
取付けるとともに、これら両センサーの検出信号
を管内挿入部分から管外に棒状部材内を介して伝
送するものである。
In response, a current meter structure as shown in Japanese Patent Application Laid-open No. 59-3315 was proposed, and in this structure,
In the pipe insertion part of the rod-shaped member inserted into the fluid transport pipe in a position perpendicular or almost perpendicular to the streamline,
a first sensor that detects the total pressure as an electrical signal;
A second sensor that detects static pressure as an electric signal is attached, and the detection signals of these two sensors are transmitted from the insertion part into the tube to the outside of the tube via the inside of the rod-shaped member.

〔考案が解決しようとする問題点〕[Problem that the invention attempts to solve]

しかしながら、上記従来構造における静圧測定
では、静圧取出し用の第2センサーとしての電流
トランスミツターS2の受圧面はダイヤフラムやベ
ローズ等から形成されており、このため、流速方
向に対し、受圧面が傾斜して設定される場合には
同受圧面近縁に乱気流が発生し、その結果、動圧
成分を取り込んで高精度の静圧測定を行なうこと
が困難であつた。
However, in the static pressure measurement with the above conventional structure, the pressure receiving surface of the current transmitter S 2 as the second sensor for taking out the static pressure is formed of a diaphragm, bellows, etc. When the surface is set to be inclined, turbulence occurs near the pressure-receiving surface, and as a result, it is difficult to take in the dynamic pressure component and measure static pressure with high precision.

本考案は上記従来の問題点に鑑みてなされたも
のであり、その目的は、空気の流れ上流側に臨む
端部を有した管体の端部間に大径筒と、管頭部に
より形成される環状スリツトを形成し、この環状
スリツトに連通して管体の最端部側に空間を延設
し、この空間と管体内部とを管体の最端部側に設
けた連通孔により連通させることにより、流速方
向に対し、静圧測定管を傾斜して設定した場合に
も動圧成分を取り込むことなく高精度に静圧を測
定することのできる流速計の静圧測定管を提供す
ることにある。
The present invention was made in view of the above-mentioned conventional problems, and its purpose is to form a large-diameter tube between the ends of the tube body, which has an end facing the upstream side of the air flow, and a tube head. A space is formed extending to the end of the tube in communication with the annular slit, and this space and the inside of the tube are connected by a communication hole provided at the end of the tube. We provide a static pressure measurement tube for a current meter that can measure static pressure with high accuracy without incorporating dynamic pressure components even when the static pressure measurement tube is set at an angle with respect to the flow velocity direction by communicating with the current flowmeter. It's about doing.

〔問題点を解決するための手段〕[Means for solving problems]

上記目的を達成するために本考案は、構造物の
通気ダクト内における空気の流速を測定する流速
計の静圧測定管であつて、静圧測定用の圧力計1
4に接続され、空気の流れ上流側に臨む端部を有
した管体3と、この管体3の端部近傍に糺着され
た大径筒2と、前記管体3の最端部全体を覆蓋す
るように形成され、端面が前記大径筒2の端面と
近接して同大径筒2の端面との間に環状スリツト
7を形成する様に設けられた管頭部6と、を備
え、前記管体3の外周縁と該管頭部6内壁との間
に前記環状スリツト7に連通し管体3の最端部側
に延設された空間8を有し、更に、この空間8と
前記管体3内部とは、前記管体3の最端部側に設
けられた連通孔5により連通されて成る流速計の
静圧測定管1から構成される。
In order to achieve the above object, the present invention provides a static pressure measuring tube for a current meter that measures the flow velocity of air in a ventilation duct of a structure, and includes a pressure gauge 1 for measuring static pressure.
4, a tube 3 having an end facing the upstream side of the air flow, a large-diameter tube 2 glued near the end of this tube 3, and the entire end of the tube 3. a pipe head 6 which is formed to cover the pipe and whose end face is close to the end face of the large diameter pipe 2 and is provided so as to form an annular slit 7 between the pipe head 6 and the end face of the large diameter pipe 2; A space 8 is provided between the outer circumferential edge of the tube body 3 and the inner wall of the tube head 6, and the space 8 communicates with the annular slit 7 and extends toward the outermost end of the tube body 3. 8 and the inside of the tube body 3 are constituted by a static pressure measuring tube 1 of a current meter, which communicates with each other through a communication hole 5 provided at the extreme end of the tube body 3.

〔作用〕[Effect]

本考案では、静圧測定管1が略風上方向に設置
され、静圧測定管1の管体3の上流側最端部に設
けられた管頭部6の外周に沿つて流れてくる空気
流は、環状スリツト7から流入することなく、空
間8内に単に静圧のみを作用させるものである。
したつて、環状スリツト7を介して管体3と管頭
部6の内壁との間に形成される空間8にはダクト
内の空気流における静圧が作用し、これによつて
連通孔5を介して計測管10内の圧力を圧力計1
4により静圧として計測するものである。
In the present invention, the static pressure measuring tube 1 is installed approximately in the windward direction, and air flows along the outer periphery of the tube head 6 provided at the most upstream end of the tube body 3 of the static pressure measuring tube 1. The flow does not enter through the annular slit 7, but merely exerts static pressure within the space 8.
Therefore, the static pressure of the air flow in the duct acts on the space 8 formed between the tube body 3 and the inner wall of the tube head 6 via the annular slit 7, thereby causing the communication hole 5 to be closed. The pressure inside the measuring tube 10 is measured through the pressure gauge 1.
4, it is measured as static pressure.

〔実施例〕〔Example〕

第1図ないし第4図は、本考案の実施例に係る
流速計の静圧測定管を主に説明するものであり、
第2図において、空気の流れ方向に対して略直角
方向を長手方向とする長矩形の計測管10が配置
され、この計測管10の中央部付近から空気の流
れ上流側に臨む端部を備えた中空円筒の管体3が
同計測管10に連通接続されている。この管体3
の上流側端部近傍には同管体3より大径の大径筒
2が膨出形成、または別体の筒体の嵌着等により
設けられている。
1 to 4 mainly explain the static pressure measuring tube of the current meter according to the embodiment of the present invention,
In FIG. 2, a long rectangular measurement tube 10 whose longitudinal direction is substantially perpendicular to the air flow direction is arranged, and has an end portion facing upstream of the air flow from near the center of the measurement tube 10. A hollow cylindrical tube body 3 is connected to the measuring tube 10 in communication. This pipe body 3
A large-diameter tube 2 having a larger diameter than the tube 3 is provided near the upstream end of the tube 3 by forming a bulge or by fitting a separate tube.

さらに、前記管体3の上流側最端部全体を覆蓋
するように管頭部6が形成されている。
Further, a tube head 6 is formed to cover the entire upstream end of the tube body 3.

この管頭部6は、上流側に対し先細りとなる先
鋭上に形成されており、例えば、キヤツプ構成等
により外部から嵌着されるようになつている。そ
して、この管頭部6の流れ下流側端面は、前記大
径筒2の上流側端面と相対向するように近接し、
両者間であつて管体3の周縁に環状スリツト7を
形成している。
The pipe head 6 is formed into a sharp point that tapers toward the upstream side, and is fitted from the outside by, for example, a cap structure. The downstream end surface of the tube head 6 is close to the upstream end surface of the large diameter tube 2 so as to face it,
An annular slit 7 is formed between the two at the periphery of the tube body 3.

本考案において特徴的なとは、上記スリツト7
に連通する空間を管体外周壁と管頭部6の内周壁
との間に流れの上流側に向かうように延設形成す
ると共に、この空間と管体内部を管体の最端部側
に設けた連通孔により連通させたことである。
What is characteristic about this invention is the above-mentioned slit 7.
A space communicating with the pipe body is formed between the outer peripheral wall of the pipe body and the inner peripheral wall of the pipe head 6 so as to extend toward the upstream side of the flow, and this space and the inside of the pipe body are provided at the endmost side of the pipe body. This is because the communication holes were made to communicate with each other.

即ち、前記管体3の外周縁と管頭部6の内壁と
の間には、空間8が前記環状スリツト7に連通し
て管体3の最端部側(流れ上流側)に延設されて
いる。更に、この空間8と管体3の内部とは前記
管体3の最端部側(流れ上流側)に設けられた連
通孔5により連通されている。なお、4は管体3
の最端部側の外周縁に設けられ空間8と管体3内
部を中間的に連通接続させる中空部である。
That is, a space 8 is provided between the outer circumferential edge of the tube body 3 and the inner wall of the tube head 6, communicating with the annular slit 7 and extending toward the most end side (flow upstream side) of the tube body 3. ing. Furthermore, this space 8 and the inside of the tubular body 3 are communicated through a communication hole 5 provided at the endmost side (flow upstream side) of the tubular body 3. In addition, 4 is tube body 3
This is a hollow portion provided at the outer peripheral edge of the outermost end of the tube body 3 to connect the space 8 and the inside of the tube body 3 in an intermediate manner.

ここにおいて、管体3の最端部側(流れ上流
側)から流れてくる空気流は環状スリツト7のス
リツト孔に作用し、これより、空間8、中空部
4、及び連通孔5により連通する管体3内に及ぼ
された圧力が静圧値と成る。
Here, the air flow flowing from the most end side (flow upstream side) of the tube body 3 acts on the slit hole of the annular slit 7, and from this, the space 8, the hollow part 4, and the communication hole 5 communicate with each other. The pressure exerted within the tube body 3 becomes a static pressure value.

図中、13,13′は圧力測定用エア管、14
は静圧測定用圧力計、10′は全圧測定用計測管、
11は計測管10′に設けた全圧測定孔、12は
横ガイド筒、14′は全圧測定用圧力計である。
In the figure, 13 and 13' are air pipes for pressure measurement, and 14
is a pressure gauge for measuring static pressure, 10' is a measuring tube for measuring total pressure,
11 is a total pressure measuring hole provided in the measuring tube 10', 12 is a horizontal guide cylinder, and 14' is a pressure gauge for measuring the total pressure.

本実施例において、管体3の端部側から流れて
くる空気流は管頭部6の先鋭部から下流側に沿つ
て、かつ、同管頭部6の外周に沿つて流れ、環状
スリツト7内から、空間8、中空部4及び連通孔
5を介して管体3の内部にダクト内の空気流にお
ける静圧が作用し、これにより、静圧測定管1が
連通された計測管10の内部圧力が前記ダクト内
の静圧と等しくなる。このように、空間8が管体
3の最端部側(流れの上流側)すなわち、上流か
らの流れに逆流する方向に延設されているので環
状スリツト7からは単に空気流の静圧が作用する
こととなる。
In this embodiment, the airflow flowing from the end side of the tube body 3 flows along the downstream side from the sharp point of the tube head 6 and along the outer periphery of the tube head 6, and flows through the annular slit 7. Static pressure in the airflow in the duct acts on the inside of the tube body 3 from inside through the space 8, the hollow part 4, and the communication hole 5, and as a result, the static pressure of the measurement tube 10 with which the static pressure measurement tube 1 is communicated acts. The internal pressure becomes equal to the static pressure within the duct. In this way, since the space 8 extends toward the end of the pipe body 3 (upstream side of the flow), that is, in the direction opposite to the flow from upstream, the annular slit 7 simply releases the static pressure of the air flow. It will work.

ここにおいて、流速の測定作業時に静圧測定管
1をダクト内で傾斜させて配置した場合であつて
も空間8内には動圧成分が作用することなく、高
精度の静圧測定を行なうこととなる。
Here, even if the static pressure measuring tube 1 is arranged at an angle in the duct during flow velocity measurement work, a dynamic pressure component does not act in the space 8, and the static pressure can be measured with high accuracy. becomes.

なお、全圧は、ダクト内の空気流を横ガイド筒
12の先端開口部から導入されて一旦滞留し、圧
力を平均化した後に全圧測定孔11を介して計測
管10′に作用し、該計測管10′内の圧力が全圧
と等しくなるものである。このようにして、計測
管10,10′内の圧力をそれぞれ静圧及び全圧
と等しくさせ、この圧力をエア管813,13′
をして圧力計14,14′により計測する。
Incidentally, the total pressure is determined by introducing the air flow in the duct through the tip opening of the horizontal guide tube 12, once stagnation, and after averaging the pressure, it acts on the measurement tube 10' through the total pressure measurement hole 11, The pressure inside the measuring tube 10' is equal to the total pressure. In this way, the pressure in the measuring tubes 10, 10' is made equal to the static pressure and the total pressure, respectively, and this pressure is
The pressure is then measured using the pressure gauges 14 and 14'.

第4図は、上記実施例に基づくダクト内の流速
方向と静圧測定管1との向きのギヤツプ、すなわ
ち、傾斜角θに対する測定値の関係を示したグラ
フ図であり、図中「〇」で示す線が従来のピトー
管による測定値を示し、「△」で示す線が実施例
に係る静圧測定管1を用いた場合の測定値を示
す。
FIG. 4 is a graph showing the gap between the flow velocity direction in the duct and the direction of the static pressure measuring tube 1 based on the above embodiment, that is, the relationship between the measured value and the inclination angle θ. The line indicated by "△" indicates the measured value using the conventional pitot tube, and the line indicated by "△" indicates the measured value using the static pressure measuring tube 1 according to the embodiment.

この実験結果に示されるように、従来のピトー
管であれば、圧力値が±5%以内の傾斜角θは−
17゜と13゜程度、つまり30゜の角度範囲で±5%の精
度を保持するのに対し、本実施例の場合、傾斜角
θが−44゜と54゜程度、つまり100゜の角度範囲で±
5%の精度を保持することができ、静圧測定管1
の空気流に対する傾きを気にすることなく安定し
た高精度の静圧の測定値を得ることが分かる。
As shown in this experimental result, in the case of a conventional Pitot tube, the inclination angle θ is - when the pressure value is within ±5%.
While accuracy of ±5% is maintained in an angle range of about 17° and 13°, that is, 30°, in this example, the inclination angle θ is about -44° and 54°, that is, an angular range of 100°. In±
Can maintain an accuracy of 5%, static pressure measuring tube 1
It can be seen that stable and highly accurate static pressure measurements can be obtained without worrying about the slope of the air flow.

なお、本実施例では、連通孔5が管体3の側面
に設けてある場合を示すが、これに限らず、例え
ば、第5図に示すように、管体3の最端部側に設
けても良い。
Although this embodiment shows a case where the communication hole 5 is provided on the side surface of the tube body 3, the communication hole 5 is not limited to this, and for example, as shown in FIG. It's okay.

〔考案の効果〕[Effect of idea]

以上説明したように、本考案に係る流速計の静
圧測定管によれば、空気の流れ上流側に臨む端部
を有した管体の端部側に大径筒と、管頭部により
形成される環状スリツトを形成し、この環状スリ
ツトに連通して管体の最端部側に空間を延設し、
この空間と管体内部とを管体の最端部側に設けた
連通孔により連通させることにより、流速方向に
対し、静圧測定管を傾斜して設定した場合にも動
圧成分を取り込むことなく高精度に静圧を測定す
ることが可能となる。
As explained above, according to the static pressure measuring tube of the current meter according to the present invention, a large diameter tube is formed on the end side of the tube body having an end facing the upstream side of the air flow, and a tube head. forming an annular slit, communicating with the annular slit and extending a space to the outermost end of the tube body;
By communicating this space with the inside of the tube through a communication hole provided at the end of the tube, dynamic pressure components can be taken in even when the static pressure measurement tube is set at an angle with respect to the flow velocity direction. This makes it possible to measure static pressure with high precision without any problems.

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

第1図は、本考案に係る流速計の静圧測定管の
実施例を示す要部断面説明図、第2図は、同静圧
測定管を用いた流速計の全体概略斜視図、第3図
は、流速計の要部拡大断面図、第4図は、本実施
例の空気流に対する傾斜角と静圧測定値の関係を
示すグラフ図、第5図は、本考案による静圧測定
管の他の実施例を示す要部断面説明図、である。 1……静圧測定管、2……大径筒、3……管
体、4……中空部、5……連通孔、6……管頭
部、7……環状スリツト、8……空間。
FIG. 1 is an explanatory cross-sectional view of the main parts showing an embodiment of the static pressure measuring tube of the current meter according to the present invention, FIG. 2 is an overall schematic perspective view of the current meter using the same static pressure measuring tube, and FIG. The figure is an enlarged cross-sectional view of the main part of the current meter, Figure 4 is a graph showing the relationship between the tilt angle and the static pressure measurement value for air flow in this embodiment, and Figure 5 is the static pressure measuring tube according to the present invention. FIG. 4 is a cross-sectional explanatory diagram of main parts showing another embodiment of the present invention. DESCRIPTION OF SYMBOLS 1... Static pressure measuring tube, 2... Large diameter tube, 3... Tube body, 4... Hollow part, 5... Communication hole, 6... Tube head, 7... Annular slit, 8... Space .

Claims (1)

【実用新案登録請求の範囲】 構造物の通気ダクト内における空気の流速を測
定する流速計の静圧測定管であつて、 静圧測定用の圧力計に接続され、空気の流れ上
流側に臨む端部を有した管体と、 この管体の端部近傍に嵌着された大径筒と、 前記管体の最端部全体を覆蓋するように形成さ
れ、端面が前記大径筒の端面と近接して同大径筒
の端面との間に環状スリツトを形成する様に設け
られた管頭部と、を備え、 前記管体の外周縁と該管頭部内壁との間に前記
環状スリツトに連通し管体の最端部側に延設され
た空間を有し、 更に、この空間と前記管体内部とは、前記管体
の最端部側に設けられた連通孔により連通されて
成る流速計の静圧測定管。
[Scope of Claim for Utility Model Registration] A static pressure measuring tube for a current meter that measures the flow velocity of air in a ventilation duct of a structure, which is connected to a pressure gauge for static pressure measurement and faces the upstream side of the air flow. a tube body having an end; a large-diameter tube fitted near the end of the tube; and a large-diameter tube formed to cover the entire extreme end of the tube, the end surface of which is an end surface of the large-diameter tube. and a tube head provided so as to form an annular slit between the tube body and the end surface of the large diameter tube, the tube head being provided so as to form an annular slit between the tube body and the end surface of the tube head, and the tube head provided between the outer circumferential edge of the tube body and the inner wall of the tube head. It has a space that communicates with the slit and extends to the endmost side of the tube, and further, this space and the inside of the tube communicate with each other through a communication hole provided at the endmost side of the tube. A static pressure measuring tube for a current meter.
JP1984181241U 1984-11-28 1984-11-28 Expired JPH0236093Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1984181241U JPH0236093Y2 (en) 1984-11-28 1984-11-28

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1984181241U JPH0236093Y2 (en) 1984-11-28 1984-11-28

Publications (2)

Publication Number Publication Date
JPS6194773U JPS6194773U (en) 1986-06-18
JPH0236093Y2 true JPH0236093Y2 (en) 1990-10-02

Family

ID=30738794

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1984181241U Expired JPH0236093Y2 (en) 1984-11-28 1984-11-28

Country Status (1)

Country Link
JP (1) JPH0236093Y2 (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS593315A (en) * 1982-06-30 1984-01-10 Nikken Syst Kk Rod-type detection terminal for measuring flow speed of fluid

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS593315A (en) * 1982-06-30 1984-01-10 Nikken Syst Kk Rod-type detection terminal for measuring flow speed of fluid

Also Published As

Publication number Publication date
JPS6194773U (en) 1986-06-18

Similar Documents

Publication Publication Date Title
US4677858A (en) Double-acting pitot tube
US5979247A (en) Flow sensor having a fixed resistance and a variable resistance
US3803921A (en) Sampling and flow measuring device
US4378696A (en) Pressure sensor for determining airspeed altitude and angle of attack
US4957007A (en) Bi-directional pressure sensing probe
JPS62159023A (en) Probe for detecting air-current data
EP0167585A1 (en) Pressure sensing instrument for aircraft.
US6044716A (en) Fluid pressure detector and air flow rate measuring apparatus using same
JPH0374570B2 (en)
US4559835A (en) Flow measuring traverse probe
CN204831400U (en) Steady voltage formula low discharge wind speed amount of wind measuring device
JPH0236093Y2 (en)
CN111044203A (en) Rotating mechanism for bidirectional dynamic pressure measurement sensor
JP3615371B2 (en) Airflow measuring device
CN212082473U (en) Matrix flowmeter
JPH0236092Y2 (en)
GB2446827A (en) A pitot-static device
CN108414133B (en) The method of friction stree is measured under high temperature indirectly
JP2537191Y2 (en) Differential pressure detector
JP3615369B2 (en) Fluid pressure detector
CN217930387U (en) Flow meter and flow detection device
JPS622495Y2 (en)
JPS6340967Y2 (en)
JPS5928326Y2 (en) differential pressure flowmeter
CN219869825U (en) Anti-blocking pressure taking head of flow sensor with high stability and wide range