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JPS6236523B2 - - Google Patents
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JPS6236523B2 - - Google Patents

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Publication number
JPS6236523B2
JPS6236523B2 JP56006836A JP683681A JPS6236523B2 JP S6236523 B2 JPS6236523 B2 JP S6236523B2 JP 56006836 A JP56006836 A JP 56006836A JP 683681 A JP683681 A JP 683681A JP S6236523 B2 JPS6236523 B2 JP S6236523B2
Authority
JP
Japan
Prior art keywords
measured
circuit
fluid
heating
temperature sensing
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
JP56006836A
Other languages
Japanese (ja)
Other versions
JPS57120816A (en
Inventor
Tatsuo Togawa
Tetsu Nemoto
Hirohisa Tsubakimoto
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Anima Corp
Original Assignee
Anima Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Anima Corp filed Critical Anima Corp
Priority to JP56006836A priority Critical patent/JPS57120816A/en
Priority to US06/422,975 priority patent/US4483200A/en
Priority to PCT/JP1982/000017 priority patent/WO1982002591A1/en
Priority to DE19823231663 priority patent/DE3231663C2/en
Publication of JPS57120816A publication Critical patent/JPS57120816A/en
Publication of JPS6236523B2 publication Critical patent/JPS6236523B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F1/00Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
    • G01F1/68Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using thermal effects

Landscapes

  • Physics & Mathematics (AREA)
  • Fluid Mechanics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Volume Flow (AREA)

Description

【発明の詳細な説明】 この発明は、電流により加熱された抵抗線を使
用して流体の流速を測定する熱線パルス流量計に
関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a hot wire pulse flow meter that measures the flow rate of a fluid using a resistance wire heated by an electric current.

被測定流体の流管の上流側において、被測定流
体を熱パルスにより加熱し、この加熱された被測
定流体を被測定流体の加熱位置から所定距離隔つ
た流管の下流側において検出し加熱時から検出時
までの時間を測定することにより、被測定流体の
流速を測定し、それに基づいて被測定流体の流量
を測定することが行なわれている。
The fluid to be measured is heated by a heat pulse on the upstream side of the flow tube of the fluid to be measured, and the heated fluid to be measured is detected at the downstream side of the flow tube at a predetermined distance from the heating position of the fluid to be measured. The flow rate of the fluid to be measured is measured by measuring the time from the time to the time of detection, and the flow rate of the fluid to be measured is measured based on this.

一方超音波を使用し、超音波の伝播時間から流
速を測定し、この流速に基づいて流量を測定する
方法も用いられている。しかし超音波は流体の組
成によつてその伝播時間が大幅に変化する難点が
ある。例えば超音波のHe中の伝播速度は0℃に
おいて19.0×104m2/S2であり、空気中ではこれ
が11.0×104m2/S2となる。これに比して、熱線
型の流量計では被測定流体の組成に影響されずに
流速の測定が可能であり、検出器も超音波の場合
に比して高精度で且つ熱線の太さや長さなどの影
響がなく配設位置で特性が定まる構造の簡単なも
のを容易に得ることが出来る。この場合、被測定
流体の流量をLml/secとし、測定用の流管の断
面積をScm2とすると、被測定流体の平均流速vは
次式で与えられる。
On the other hand, a method is also used in which ultrasonic waves are used, the flow velocity is measured from the propagation time of the ultrasonic waves, and the flow rate is measured based on this flow velocity. However, ultrasonic waves have the disadvantage that their propagation time varies considerably depending on the composition of the fluid. For example, the propagation velocity of ultrasonic waves in He is 19.0×10 4 m 2 /S 2 at 0° C., and in air it is 11.0×10 4 m 2 /S 2 . In contrast, hot wire flowmeters can measure flow velocity without being affected by the composition of the fluid being measured, and the detectors are more accurate than those using ultrasonic waves, and the thickness and length of the hot wire can be measured. It is possible to easily obtain a simple structure whose characteristics are determined by the installation position without being affected by the size or the like. In this case, assuming that the flow rate of the fluid to be measured is Lml/sec and the cross-sectional area of the flow tube for measurement is Scm2 , the average flow velocity v of the fluid to be measured is given by the following equation.

v=L/S(cm/sec) (1) 流管内の上流側に設けられた被測定流体の加熱
部と、流管の下流側に設けられた感温部間の距離
をd(cm)とし、加熱部における被測定流体への
加熱時から、感温部における加熱された被測定流
体の検出迄に要する時間をTとすると、次式が成
立する。
v=L/S (cm/sec) (1) The distance between the heating part of the fluid to be measured installed on the upstream side of the flow tube and the temperature sensing part installed on the downstream side of the flow tube is d (cm) If T is the time required from the heating of the fluid to be measured in the heating section to the detection of the heated fluid to be measured in the temperature sensing section, then the following equation holds true.

T=1/LS.d(sec) (2) 加熱部の発熱体として、直径D、長さlのW線
を使用し、W線の密度をP(g/cm3)その熱伝導
率をCp(cal/g〓)抵抗値をR、印加電圧をV
その通電時間をtとすると、被測定流体に与えら
れる熱量△Tは、次式で与えられる。
T=1/LS.d (sec) (2) Use a W wire with diameter D and length l as the heating element in the heating section, and the density of the W wire is P (g/cm 3 ) and its thermal conductivity is Cp (cal/g〓) resistance value is R, applied voltage is V
When the current application time is t, the amount of heat ΔT given to the fluid to be measured is given by the following equation.

(2)式で明らかなように、被測定流体の流量Lが
増加して行くと、これに反比例して時間Tが減少
して行く。このため、特にその被測定流体の流量
が大幅に変化するような測定系においては、加熱
部においての被測定流体の加熱時間周期の設定が
困難となる。即ちこの加熱時間周期を余り大きく
設定すると、被測定流体の流量の変化に正確に追
従した測定が出来なくなる。一方、加熱時間周期
を余り短かくすると単位時間ごとに流管の下流側
で検出される流体に前の時間周期における加熱の
影響が与えられて、その検出が不正確になる。
As is clear from equation (2), as the flow rate L of the fluid to be measured increases, the time T decreases in inverse proportion to this. Therefore, especially in a measurement system where the flow rate of the fluid to be measured changes significantly, it is difficult to set the heating time period of the fluid to be measured in the heating section. That is, if this heating time period is set too long, it will not be possible to perform measurements that accurately follow changes in the flow rate of the fluid to be measured. On the other hand, if the heating time period is made too short, the fluid detected on the downstream side of the flow tube for each unit time will be affected by the heating in the previous time period, making the detection inaccurate.

この発明は、この従来の熱線パルス流量計にお
ける難点を解決し、被測定流体の流量に対応して
加熱部における発熱時間周期を変化可能とし、広
い範囲の流量変化に応じて、常に正確で効率のよ
い流量測定が可能な熱線パルス流量計を提供する
ものである。
This invention solves the problems with conventional hot-wire pulse flowmeters, makes it possible to change the heat generation time period in the heating section in response to the flow rate of the fluid being measured, and allows for constant accuracy and efficiency in response to a wide range of flow rate changes. The present invention provides a hot wire pulse flowmeter that can measure flow rates with good accuracy.

この発明においては、被測定流路内の被測定流
体に対して所定の位置において瞬時的に被測定流
体を加熱する加熱手段が設けられ、この加熱手段
により加熱された被測定流体の通過位置に感温素
子が設けられる。前記感温素子に接続され、加熱
された被測定流体が通過するのを検出する感温回
路部が設けられる。また前記加熱手段による加熱
から前記感温回路部の検出までの時間を計測し、
前記感温回路部の検出から前記計測時間と等しい
時間だけ更に経過後に前記加熱手段を駆動する時
間設定回路が設けられ、この時間設定回路による
加熱手段の駆動周期に対応して前記被測定流体の
流量を測定する手段が設けられる。また前記被測
定流体の流量が所定値以下になつたことを検出す
るタイマ手段が設けられ、そのタイマ手段の検出
中、前記加熱手段を一定周期で駆動する。(この
ように被測定流体の流量が所定値以下になつた場
合、例えば流れがほゞ止つたような場合にも一定
周期(例えば10Hz程度)で加熱手段を駆動してい
ると、流れが急に再開された場合にも即応してそ
の流量を測定することができる。) 以下、この発明の熱線パルス流量計をその実施
例に基づき、図面を使用して詳細に説明する。
In this invention, a heating means is provided for instantaneously heating the fluid to be measured at a predetermined position in the flow path to be measured, and the fluid to be measured heated by the heating means passes through the fluid. A temperature sensitive element is provided. A temperature sensing circuit section is provided which is connected to the temperature sensing element and detects passage of the heated fluid to be measured. Also, measuring the time from heating by the heating means to detection of the temperature sensitive circuit section,
A time setting circuit is provided for driving the heating means after a period of time equal to the measurement time has elapsed since the detection by the temperature sensing circuit, and the temperature of the fluid to be measured is adjusted in accordance with the driving cycle of the heating means by the time setting circuit. Means are provided for measuring the flow rate. Further, a timer means is provided for detecting that the flow rate of the fluid to be measured has become less than a predetermined value, and while the timer means is detecting, the heating means is driven at a constant cycle. (If the flow rate of the fluid to be measured falls below a predetermined value, for example, even if the flow has almost stopped, if the heating means is driven at a constant cycle (for example, about 10 Hz), the flow will suddenly stop.) Even when the flow rate is restarted, the flow rate can be measured immediately.) Hereinafter, the hot wire pulse flow meter of the present invention will be described in detail based on embodiments thereof and with reference to the drawings.

第1図はこの発明の構成を示す図で、流管11
内に被測定流体Fが導入され、この流管11の上
流側において、流管11内周面に被測定流体Fの
流れ方向に直角に乱流発生体12が設けられる。
この乱流発生体12は、例えば被測定流体Fの流
れに直角な面上に、金属線でメツシユ状体が形成
された構成を有する。
FIG. 1 is a diagram showing the configuration of the present invention, in which a flow tube 11
A fluid F to be measured is introduced into the flow tube 11, and a turbulence generator 12 is provided on the inner peripheral surface of the flow tube 11 at right angles to the flow direction of the fluid F to be measured on the upstream side of the flow tube 11.
The turbulence generator 12 has a structure in which a mesh-like body is formed of metal wire on a surface perpendicular to the flow of the fluid F to be measured, for example.

流管11に導入される被測定流体Fは一般には
層流で流れに直角な面内で、或る速度分布を有す
る。この導入された層流状の被測定流体Fは、こ
の乱流発生体により乱流となり、流れに直角な面
内で一様な平均速度を有する状態になる。
The fluid F to be measured introduced into the flow tube 11 is generally laminar and has a certain velocity distribution in a plane perpendicular to the flow. The introduced laminar fluid F to be measured becomes a turbulent flow due to the turbulence generator, and has a uniform average velocity in a plane perpendicular to the flow.

流管11内においてこの乱流発生体12の下流
側に発熱体13が、流管11の直径方向に張りわ
たされる。この発熱体13は、例えば直径5μの
W線で形成され、この発熱体13から被測定流体
を加熱する熱パルスが被測定流体に与えられる。
即ち、発熱回路部14が設けられ、この発熱回路
部14では加熱パルス幅設定回路10から発生し
た所定のパルス幅の加熱パルスSHによつて加熱
回路18が励起され、励起された加熱回路18に
接続された発熱体13が発熱して被測定流体がこ
の熱パルスによつて加熱される。
A heating element 13 is placed in the flow tube 11 on the downstream side of the turbulence generator 12 in the diametrical direction of the flow tube 11 . The heating element 13 is formed of a W wire having a diameter of 5 μm, for example, and a heat pulse for heating the fluid to be measured is applied from the heating element 13 to the fluid to be measured.
That is, a heat generating circuit section 14 is provided, and in this heat generating circuit section 14, a heating circuit 18 is excited by a heating pulse S H of a predetermined pulse width generated from a heating pulse width setting circuit 10, and the heated heating circuit 18 is excited. The heating element 13 connected to generates heat, and the fluid to be measured is heated by this heat pulse.

流管11に対してこの発熱回路部14の下流側
には感温回路部15が設けられる。感温回路部1
5においては、感温素子19の出力端子間に感温
回路20が接続され、この感温回路20の出力端
には増幅整形回路21が接続されて、この増幅整
形回路21の出力端にフイルター9が接続され
る。感温素子19で検出された加熱された被測定
流体に対応したパルスが増幅整形され、フイルタ
ー9により直流分が阻止され、フイルター9の出
力信号は正帰還回路8を経て、シユミツト回路7
に与えられ、シユミツト回路7の出力端から作動
信号SDが得られる。
A temperature sensing circuit section 15 is provided downstream of the heat generating circuit section 14 with respect to the flow tube 11 . Temperature sensing circuit section 1
5, a temperature sensing circuit 20 is connected between the output terminals of the temperature sensing element 19, an amplification shaping circuit 21 is connected to the output terminal of this temperature sensing circuit 20, and a filter is connected to the output terminal of this amplification shaping circuit 21. 9 is connected. The pulse corresponding to the heated fluid to be measured detected by the temperature sensing element 19 is amplified and shaped, the DC component is blocked by the filter 9, and the output signal of the filter 9 passes through the positive feedback circuit 8 and is sent to the Schmitt circuit 7.
, and an actuation signal S D is obtained from the output terminal of the Schmitt circuit 7.

増幅整形回路21の出力段には図示していない
比較回路が接続され、この比較回路に与えられて
いる基準信号設定器からの基準信号と検出パルス
Sが比較され、これが基準値を越えると、シユ
ミツト回路7からは、作動信号SDが発せられ
る。この作動信号SDによつて時間設定回路16
が駆動され、所定時間後に時間設定回路16から
時間設定信号STが発せられる。
A comparison circuit (not shown) is connected to the output stage of the amplification and shaping circuit 21, and the detection pulse S S is compared with the reference signal from the reference signal setter given to this comparison circuit, and if this exceeds the reference value, , the Schmitt circuit 7 issues an actuation signal S D. The time setting circuit 16 is controlled by this operating signal S D.
is driven, and after a predetermined time, a time setting signal S T is generated from the time setting circuit 16.

被測定流体は例えば呼気及び吸気に伴なうもの
などあり、いずれの場合の測定にも対応出来るよ
うに被測定流体に対しては発熱回路部14により
周期的に発熱体13から加熱パルスが与えられて
加熱が行なわれている。即ちパルス発生器5から
は例えば10Hzのパルス信号がスイツチ回路6を経
てパルス幅設定回路10に与えられていて、常時
は加熱回路18へ、このパルス発生器5のパルス
信号に対応した加熱パルスSHが発せられてい
る。パルス幅設定回路10の出力端にパルスカウ
ンタ演算回路3が接続され、パルスカウンタ演算
回路3の出力端に表示器2が接続されて、加熱パ
ルスSHによる加熱回路18の起動周期と対応し
て被測定流体の流量が演算表示されるような構成
となつている。
The fluid to be measured includes, for example, that associated with exhalation and inhalation, and the heating circuit section 14 periodically applies heating pulses from the heating element 13 to the fluid to be measured so that measurement can be carried out in either case. heating is carried out. That is, a pulse signal of, for example, 10 Hz is supplied from the pulse generator 5 to the pulse width setting circuit 10 via the switch circuit 6, and the heating pulse S corresponding to the pulse signal of the pulse generator 5 is normally supplied to the heating circuit 18. H is emitted. A pulse counter arithmetic circuit 3 is connected to the output end of the pulse width setting circuit 10, and a display 2 is connected to the output end of the pulse counter arithmetic circuit 3 . The structure is such that the flow rate of the fluid to be measured is calculated and displayed.

被測定流体の流量が測定レンジの最小流量を僅
か越えると、一致回路26からの時間設定信号S
Tによつて加熱パルス発生回路部17が駆動され
るように構成されている。即ち一致回路26の出
力端はパルス幅設定回路10に接続されると共
に、タイマー4に接続され、このタイマー4の出
力端はスイツチ回路6のゲート端子に接続され
る。タイマー4は時間設定信号STが要求される
最小流量に対応する周期より僅かに小さな値にな
ると、ゲート信号Sgを発してスイツチ回路6の
ゲートを閉じる。時間設定回路16には例えば、
加熱パルス発生回路部17のパルス幅設定回路1
0からの加熱パルスSHによつて計数が開始され
例えば発振周波数が20KHzの発振器25の発振
信号を計数するアツプダウンカウンタ24が設け
られている。このアツプダウンカウンタ24は、
被測定流体が発熱体13と検出体19間を流れる
時間の間計数を持続し、感温回路部15からの作
動信号SDによつてダウンカウントを行なう。こ
のダウンカウント数が加熱パルスSHで計数が開
始されてすでに完了している計数値に一致したこ
とが、カウンタ24の出力端に接続された一致回
路26で検出されると、時間設定回路16から時
間設定信号STが発せられる。
When the flow rate of the fluid to be measured slightly exceeds the minimum flow rate of the measurement range, the time setting signal S from the matching circuit 26 is activated.
The heating pulse generating circuit section 17 is configured to be driven by T. That is, the output terminal of the matching circuit 26 is connected to the pulse width setting circuit 10 and also to the timer 4, and the output terminal of the timer 4 is connected to the gate terminal of the switch circuit 6. The timer 4 issues a gate signal S g to close the gate of the switch circuit 6 when the time setting signal S T reaches a value slightly smaller than the period corresponding to the required minimum flow rate. For example, the time setting circuit 16 includes:
Pulse width setting circuit 1 of heating pulse generation circuit section 17
An up-down counter 24 is provided, which starts counting by the heating pulse S H from 0 and counts the oscillation signal of an oscillator 25 having an oscillation frequency of 20 KHz, for example. This up-down counter 24 is
Counting is continued during the time that the fluid to be measured flows between the heating element 13 and the detection element 19, and a down count is performed in response to the activation signal S D from the temperature sensing circuit section 15. When the coincidence circuit 26 connected to the output terminal of the counter 24 detects that this downcount number matches the count value that has already been completed after counting started with the heating pulse SH , the time setting circuit 16 A time setting signal S T is issued from.

第2図の実施例に示すように、スイツチ回路6
の出力信号Snもしくは時間設定信号STがトラン
ジスタ30のベースTpに与えられ、トランジス
タ30から発せられる駆動信号Spによつてパル
ス幅設定回路10から所定パルス幅の加熱パルス
Hが発せられる。この加熱パルスSHがトランジ
スタ32のベースに与えられて、トランジスタ3
2のエミツタにそのベースが接続されているトラ
ンジスタ33が導通状態となり、そのエミツタと
アース間に接続されている発熱体13に瞬時的に
加熱電流が流れる。
As shown in the embodiment of FIG.
An output signal S n or a time setting signal S T is applied to the base T p of the transistor 30, and a heating pulse S H of a predetermined pulse width is emitted from the pulse width setting circuit 10 by the drive signal S p emitted from the transistor 30 . It will be done. This heating pulse S H is applied to the base of the transistor 32, and the transistor 3
Transistor 33, whose base is connected to the emitter of transistor 2, becomes conductive, and a heating current instantaneously flows through heating element 13, which is connected between its emitter and ground.

前述のように常時はパルス発生器5からのパル
ス信号に対応したスイツチ回路6の出力信号Sn
によりパルス幅設定回路10が駆動され、時間設
定信号STが最小流量に対応する周期より僅かに
小さくなると、ゲート信号Sgによりスイツチ回
路6がゲートを閉じて、パルス幅設定回路10は
時間設定信号STによつて駆動される。
As mentioned above, the output signal S n of the switch circuit 6 corresponding to the pulse signal from the pulse generator 5 is always
The pulse width setting circuit 10 is driven, and when the time setting signal S T becomes slightly smaller than the period corresponding to the minimum flow rate, the gate signal S g causes the switch circuit 6 to close the gate, and the pulse width setting circuit 10 starts setting the time. Driven by signal S T .

発熱体13が加熱されると、その加熱時に発熱
体13部分を流れる被測定流体が加熱される。こ
の加熱された被測定流体が感温素子19部分を通
過すると、感温素子19が加熱されて、その抵抗
値が上昇する。この感温素子19を一辺とするブ
リツジ34が構成され、そのブリツジ34の検出
端子間に増幅器35が接続される。被測定流体に
温度変化が生じてブリツジ34が不平衡状態にな
ると、増幅器35から検出信号SCが発せられ
る。
When the heating element 13 is heated, the fluid to be measured flowing through the heating element 13 is heated at the time of heating. When this heated fluid to be measured passes through the temperature sensing element 19, the temperature sensing element 19 is heated and its resistance value increases. A bridge 34 having one side of this temperature sensing element 19 is constructed, and an amplifier 35 is connected between detection terminals of the bridge 34. When the bridge 34 becomes unbalanced due to a temperature change in the fluid to be measured, the amplifier 35 generates a detection signal S C .

第1図の実施例では感温素子19は第1、第2
の感温素子19−1,19−2からなり、それぞ
れが互にその位置をずらして配設されている。例
えば呼気の測定を行なう場合に、第1の感温素子
19−1に対してずらして配設された第2の感温
素子19−2が呼気に対して人体から与えられる
熱量を分離検出するので、感温回路20で被測定
流体に対して人体から与えられる熱量の影響を除
去した測定を行なうことが出来る。又呼気及び吸
気を測定する場合には、第5図に示すように発熱
体13を狭んで両側に二組の感温素子19,1
9′を配設すればよい。この検出信号SCが抵抗3
7とコンデンサ38よりなる積分回路36に与え
られ、積分回路36の出力は、コンデンサ39に
与えられて、検出信号SC中の直流分が阻止され
る。直流分が阻止された検出信号SCが増幅器4
0,41により増幅整形されて、増幅器41の出
力端に整形された検出パルスSCが得られる。こ
の検出パルスSCが感温回路部15の比較増幅器
42の非反転入力端子に与えられる。
In the embodiment shown in FIG.
The temperature sensing elements 19-1 and 19-2 are arranged with their positions shifted from each other. For example, when measuring exhaled breath, the second temperature sensing element 19-2, which is arranged offset from the first temperature sensing element 19-1, separates and detects the amount of heat given by the human body to the exhaled breath. Therefore, the temperature sensing circuit 20 can perform measurements in which the influence of the amount of heat given by the human body to the fluid to be measured is removed. In addition, when measuring exhalation and inhalation, two sets of temperature sensing elements 19, 1 are placed on both sides of the heating element 13, as shown in FIG.
9' may be provided. This detection signal S C is
7 and a capacitor 38, and the output of the integrating circuit 36 is fed to a capacitor 39 to block the DC component in the detection signal S.sub.C. The detection signal S C with the DC component blocked is sent to the amplifier 4
0,41, and a shaped detection pulse S C is obtained at the output end of the amplifier 41. This detection pulse S C is applied to the non-inverting input terminal of the comparison amplifier 42 of the temperature sensing circuit section 15 .

一方、増幅器41の出力端子は、比較増幅器4
3の非反転入力端子に接続され、比較増幅器43
の出力端子には、ダイオード44の陰極側が接続
される。ダイオード44の陽極側はコンデンサ4
5の一端に接続され、このコンデンサ45の他端
は接地される。ダイオード44の陽極側は、比較
増幅器46の非反転端子に接続され、比較増幅器
43と46との非反転端子が互に接続される。比
較増幅器46の出力端は抵抗47及び48を介し
て可変抵抗器49の可変端子に接続される。抵抗
47と48の接続点は比較増幅器42の反転入力
端に接続される。
On the other hand, the output terminal of the amplifier 41 is connected to the comparator amplifier 4
3, and is connected to the non-inverting input terminal of the comparison amplifier 43.
The cathode side of the diode 44 is connected to the output terminal of the diode 44 . The anode side of the diode 44 is connected to the capacitor 4
5, and the other end of this capacitor 45 is grounded. The anode side of the diode 44 is connected to the non-inverting terminal of the comparison amplifier 46, and the non-inverting terminals of the comparison amplifiers 43 and 46 are connected to each other. The output terminal of comparison amplifier 46 is connected to the variable terminal of variable resistor 49 via resistors 47 and 48. The connection point between resistors 47 and 48 is connected to the inverting input terminal of comparator amplifier 42.

ダイオード44の陽極側にはダイオード50の
陰極側が接続され、このダイオード50の陽極側
はマルチバイブレータ51の出力端に接続され
る。比較増幅器42の出力端には、反転回路52
が接続されている。
The anode side of the diode 44 is connected to the cathode side of the diode 50, and the anode side of the diode 50 is connected to the output end of the multivibrator 51. An inverting circuit 52 is connected to the output terminal of the comparison amplifier 42.
is connected.

比較増幅器41の出力端に得られる検出パルス
Cが予め設定した所定値より小さな波高値であ
ると、比較増幅器43の出力信号は所定値より小
さく、ダイオード44は導通状態にある。ダイオ
ード44の導通状態では、コンデンサ45の電荷
が放電し、比較増幅器46の出力端には負電圧が
現われて、反転回路52の出力端には作動信号S
Dが発生しない。
If the detection pulse S C obtained at the output terminal of the comparator amplifier 41 has a peak value smaller than a predetermined value, the output signal of the comparator amplifier 43 is smaller than the predetermined value, and the diode 44 is in a conductive state. When the diode 44 is conductive, the charge in the capacitor 45 is discharged, a negative voltage appears at the output terminal of the comparator amplifier 46, and the operating signal S appears at the output terminal of the inverting circuit 52.
D does not occur.

しかし、検出パルスSCの波高値が所定の設定
値を越えると、ダイオード44が遮断状態とな
り、比較増幅器42の反転端子に所定の基準電圧
が設定され、反転回路52の出力端子に作動信号
Dが発生する。マルチバイブレータ51の励起
端子t1にリセツト信号を与えると、コンデンサ4
5に正パルスが印加されて、リセツト操作を行な
うことが出来る。
However, when the peak value of the detection pulse S C exceeds a predetermined set value, the diode 44 is cut off, a predetermined reference voltage is set at the inverting terminal of the comparator amplifier 42 , and the operating signal S is sent to the output terminal of the inverting circuit 52 . D occurs. When a reset signal is applied to the excitation terminal t1 of the multivibrator 51, the capacitor 4
A positive pulse is applied to 5 to perform a reset operation.

作動信号SDは、第3図に示すように、NOR回
路60の入力端子に与えられ、NOR回路60の
出力端子はNOR回路61の一つの入力端子に接
続される。NOR回路61の出力端子はNOR回路
60の他の入力端子に接続される。NOR回路6
1の出力端子はNOR回路62の一つの入力端子
に接続される。NOR回路62の出力端子はNOR
回路63の一つの入力端子に接続され、この
NOR回路63の出力端子はNOR回路62の他の
入力端子に接続されている。NOR回路63の他
の入力端子には、NAND回路64の出力端子が接
続され、このNAND回路64の一つの入力端子に
コンデンサ65の一端が接続され、コンデンサ6
5の他端は接地される。
The actuation signal S D is applied to the input terminal of a NOR circuit 60, and the output terminal of the NOR circuit 60 is connected to one input terminal of a NOR circuit 61, as shown in FIG. An output terminal of NOR circuit 61 is connected to another input terminal of NOR circuit 60. NOR circuit 6
1 output terminal is connected to one input terminal of the NOR circuit 62. The output terminal of the NOR circuit 62 is NOR
connected to one input terminal of the circuit 63;
An output terminal of the NOR circuit 63 is connected to another input terminal of the NOR circuit 62. The output terminal of a NAND circuit 64 is connected to the other input terminal of the NOR circuit 63, and one end of a capacitor 65 is connected to one input terminal of this NAND circuit 64.
The other end of 5 is grounded.

NAND回路64のコンデンサ65が接続される
端子には、抵抗66を介して所定の電源が印加さ
れる。コンデンサ65の両極板間にはスタートス
イツチ67が接続されている。NOR回路62の
出力端には反転回路68の入力端子が接続されこ
の反転回路68の出力端子はNAND回路69の一
つの入力端子に接続される。NAND回路69の他
の入力端子には発振器25から20KHzの基準信
号が与えられている。反転回路68の出力端子が
他の反転回路70を介してNAND回路71の一つ
の入力端子に接続される。このNAND回路71の
入力端子には発振器25から20KHzの基準信号
が与えられる。
A predetermined power supply is applied via a resistor 66 to a terminal of the NAND circuit 64 to which a capacitor 65 is connected. A start switch 67 is connected between the two plates of the capacitor 65. The output terminal of the NOR circuit 62 is connected to the input terminal of an inverting circuit 68, and the output terminal of the inverting circuit 68 is connected to one input terminal of a NAND circuit 69. A 20 KHz reference signal is applied from the oscillator 25 to the other input terminal of the NAND circuit 69. An output terminal of the inverting circuit 68 is connected to one input terminal of a NAND circuit 71 via another inverting circuit 70. A 20 KHz reference signal is applied from the oscillator 25 to the input terminal of this NAND circuit 71.

NAND回路69及び71のそれぞれの出力端子
は、NOR回路72のそれぞれの入力端子に接続
される。このNOR回路72の出力端子は、直列
に接続されたアツプダウンカウンタ73,74及
び75のクロツク端子にそれぞれ接続される。又
カウンタ73,74及75のそれぞれの制御端子
cには、反転回路68の出力端子が接続されて
いる。
The respective output terminals of the NAND circuits 69 and 71 are connected to the respective input terminals of the NOR circuit 72. The output terminal of this NOR circuit 72 is connected to the clock terminals of up-down counters 73, 74 and 75 connected in series, respectively. Further, the output terminal of the inverting circuit 68 is connected to each control terminal t c of the counters 73 , 74 and 75 .

カウンタ73,74及び75の各出力端子tp
,tp2,tp3及び各制御端子が一括された端子
が、NOR回路76の入力端子にそれぞれ接続さ
れる。このNOR回路76の出力端子はNOR回路
77を介してNAND回路64の入力端子の一つに
接続されている。
Each output terminal t p of counters 73, 74 and 75
1 , t p2 , t p3 and each control terminal are connected to the input terminal of the NOR circuit 76, respectively. The output terminal of this NOR circuit 76 is connected to one of the input terminals of the NAND circuit 64 via a NOR circuit 77.

始動時においては、第3図のスイツチ67が投
入され、同時に第2図のトランジスタ30のベー
スTpに対してスイツチ回路6の出力信号Snが与
えられてパルス幅設定回路10から加熱パルスS
Hが発せられる。この加熱パルスSHがNOR回路
61の入力端子T1に与えられるので、NOR回路
62の出力端子の信号の論理値が“1”となる。
反転回路68を介して、各カウンタ73,74,
75の制御端子tcの信号の論理値は“0”に設
定され、各カウンタ73,74,75はクロツク
端子に与えられる発振器25の20KHzの信号を
計数して行く。
At the time of starting, the switch 67 shown in FIG. 3 is turned on, and at the same time, the output signal S n of the switch circuit 6 is applied to the base T p of the transistor 30 shown in FIG.
H is emitted. Since this heating pulse S H is applied to the input terminal T 1 of the NOR circuit 61, the logic value of the signal at the output terminal of the NOR circuit 62 becomes "1".
Each counter 73, 74,
The logical value of the signal at the control terminal tc of the clock terminal 75 is set to "0", and each counter 73, 74, 75 counts the 20 KHz signal of the oscillator 25 applied to the clock terminal.

被測定流体に与えられた熱パルスが感温素子1
9で検出されて、反転回路52から作動信号SD
が発せられると、この作動信号SDは、NOR回路
60の入力端子T2に与えられる。然る時には、
NOR回路62の出力端子の信号の論理値は
“0”となり、反転回路68を介して、各カウン
タ73,74,75の制御端子tcの信号の論理
値が“1”となつて、各カウンタはダウンカウン
ト動作に制御されクロツク端子に与えられる信号
で、すでに計数されている計数値をダウンカウン
トして行く。
The heat pulse given to the fluid to be measured is transmitted to the temperature sensing element 1.
9 and the activation signal S D is output from the inverting circuit 52.
When the activation signal S D is issued, this activation signal S D is applied to the input terminal T 2 of the NOR circuit 60 . When the time comes,
The logic value of the signal at the output terminal of the NOR circuit 62 becomes "0", and the logic value of the signal at the control terminal t c of each counter 73, 74, 75 becomes "1" via the inverting circuit 68. The counter is controlled to perform a down-count operation, and uses a signal applied to the clock terminal to down-count the already counted value.

すでに計数されている計数値が計数され尽して
出力端子tp1,tp2,tp3の信号がすべて論理値
“0”となると、この時すでに制御端子tcの信号
の論理値は“0”となつているので、これが
NOR回路76で検知され、NOR回路76の出力
端に時間設定信号STが現われる。この時間設定
信号STはタイマー4に与えられ、時間設定信号
Tの周期が最小流量に対応する周期より僅かに
小さくなると、タイマー4はゲート信号Sgを発
する。このゲート信号Sgが発せられるとこれが
第3図には図示していない第1図のスイツチ回路
6に与えられてそのゲートを閉じパルス発生器5
からのパルス信号のパルス幅設定回路10への入
力を阻止し、時間設定信号STがトランジスタ3
0のベースに入力信号として与えられて、この時
間設定信号STによつて加熱パルス発生回路17
が駆動されて、加熱回路18からの加熱パルスに
より被測定流体が加熱される状態となる。
When the already counted count value is exhausted and the signals at the output terminals t p1 , t p2 , and t p3 all become logic value "0", the logic value of the signal at the control terminal t c has already become "0". ”, so this is
It is detected by the NOR circuit 76, and a time setting signal S T appears at the output terminal of the NOR circuit 76. This time setting signal S T is given to the timer 4, and when the period of the time setting signal S T becomes slightly smaller than the period corresponding to the minimum flow rate, the timer 4 issues a gate signal S g . When this gate signal S g is generated, it is applied to the switch circuit 6 of FIG. 1 (not shown in FIG. 3), which closes the gate to the pulse generator 5.
The input of the pulse signal from the transistor 3 to the pulse width setting circuit 10 is blocked, and the time setting signal S T is input to the pulse width setting circuit 10.
This time setting signal S T is applied as an input signal to the base of the heating pulse generating circuit 17.
is driven, and the fluid to be measured is heated by the heating pulse from the heating circuit 18.

この実施例においては、加熱パルスが発せられ
て、感温回路部15でそれが検出される迄の時間
Tの2倍の間隔で時間設定信号STに基づく加熱
パルスが遂次発せられる。時間設定信号STの周
期が最小流量に対応する周期より僅かに増加する
と、タイマー4はゲート信号Sgによりスイツチ
回路6のゲートを開いて、加熱回路18はパルス
発生器5からのパルス信号に基いて加熱されるこ
とになる。
In this embodiment, heating pulses based on the time setting signal S T are successively emitted at intervals twice the time T from when the heating pulse is emitted until it is detected by the temperature sensitive circuit section 15 . When the period of the time setting signal S T increases slightly from the period corresponding to the minimum flow rate, the timer 4 opens the gate of the switch circuit 6 by the gate signal S g , and the heating circuit 18 responds to the pulse signal from the pulse generator 5. It will be heated based on the temperature.

以上のようにこの発明によると、常時は被測定
流体はパルス発生器5のパルス信号により周期的
に加熱され、呼気吸気いずれの流量測定にも対応
可能な状態とされ、時間設定信号STの周期が所
定値以下になると被測定流体はこの周期で加熱さ
れて感温回路部15で検出される。時間設定信号
Tは発熱体13を加熱により感温回路部15で
加熱された流体を検出するまでの時間Tの2倍の
間隔に設定されることにより発熱体13及び感温
素子19に十分冷却する時間を与えることが可能
であり、被測定流体の温度検出には、前の加熱パ
ルスの加熱の温度の悪影響が生じ難いので、呼吸
流量計のように比較的流量が大きく、上記時間T
が短い場合にも常に高精度の流量測定が可能であ
り、高流量部のダイナミツクレンジを大幅に広げ
ることができる。第4図はこの発明の熱線パルス
流量計で得られた流量lと加熱時から検出時まで
の時間との関係を示すもので、広い流量について
直線性がきわめて良好であることが示されてい
る。
As described above, according to the present invention, the fluid to be measured is regularly heated periodically by the pulse signal of the pulse generator 5, and is in a state that can be used for both exhalation and inspiration flow measurement, and the time setting signal S T When the cycle becomes equal to or less than a predetermined value, the fluid to be measured is heated at this cycle and detected by the temperature sensing circuit section 15. The time setting signal S T is set at an interval twice the time T required for detecting the heated fluid in the temperature sensing circuit section 15 by heating the heating element 13, so that it is sufficient for the heating element 13 and the temperature sensing element 19. It is possible to give time for cooling, and the temperature detection of the measured fluid is unlikely to be adversely affected by the temperature of the heating of the previous heating pulse.
Highly accurate flow measurement is always possible even when the flow rate is short, and the dynamic range of high flow areas can be greatly expanded. Figure 4 shows the relationship between the flow rate l obtained with the hot-wire pulse flowmeter of the present invention and the time from heating to detection, and shows that linearity is extremely good over a wide range of flow rates. .

以上詳細に説明したように、この発明によると
被測定流体に対しての加熱パルスの印加間隔が被
測定流体の流速、流量に追従して自動的に変化さ
れるので、流量変動の激しい流体、例えば呼吸の
流量の測定に対しても効率のよい測定が可能であ
る。
As explained in detail above, according to the present invention, the application interval of heating pulses to the fluid to be measured is automatically changed in accordance with the flow velocity and flow rate of the fluid to be measured, so that fluids with large flow fluctuations, For example, it is possible to efficiently measure the respiratory flow rate.

従つて、消費電力も少なく感温回路部での検出
が前回の加熱パルスによる悪影響を受けず、流体
の種類、温度及び周囲温度の影響を受けず、誤差
の少ない正確な被測定流体の流量の測定が可能と
なる。被測定流体の流量が所定値(例えば測定レ
ンジの最小値)以下でも固定周期で加熱手段が駆
動されているので、流量が所定値以上に急変した
場合にも即応してその変化した流量が測定でき
る。従つて流れが一時止まり急に再開される呼
気、吸気の測定にも適用することが可能となる。
また定量的検出時における校正も検出系の幾何学
的寸法のみに依存して簡単である。測定流量は低
流量から高流量まで広範囲に及び、例えば人間の
呼吸気量の測定も充分に可能である。
Therefore, the power consumption is low, and the detection in the temperature sensing circuit is not affected by the previous heating pulse, and is not affected by the type of fluid, temperature, or ambient temperature, and it is possible to accurately measure the flow rate of the fluid to be measured with little error. Measurement becomes possible. Even if the flow rate of the fluid to be measured is below a predetermined value (for example, the minimum value of the measurement range), the heating means is driven at a fixed cycle, so even if the flow rate suddenly changes beyond the predetermined value, the changed flow rate can be measured immediately. can. Therefore, it can also be applied to measurements of expiration and inspiration in which the flow temporarily stops and then suddenly resumes.
Also, calibration during quantitative detection is simple as it depends only on the geometrical dimensions of the detection system. The measured flow rate ranges over a wide range from a low flow rate to a high flow rate, and it is sufficiently possible to measure, for example, human respiratory volume.

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

第1図はこの発明の熱線パルス流量計の実施例
の全体の構成を示すブロツク図、第2図、第3図
はそれぞれこの発明の熱線パルス流量計の実施例
の主要部の回路図、第4図はこの発明の熱線パル
ス流量計で得られる被測定流体の流量と検出時間
との関係を示す図、第5図はこの発明の熱線パル
ス流量計の実施例における発熱体と検出体の配設
状態を示す図である。
FIG. 1 is a block diagram showing the overall configuration of an embodiment of the hot-wire pulse flowmeter of the present invention, and FIGS. 2 and 3 are circuit diagrams of the main parts of the embodiment of the hot-wire pulse flowmeter of the present invention, respectively. Fig. 4 is a diagram showing the relationship between the flow rate of the fluid to be measured and the detection time obtained by the hot-wire pulse flowmeter of the present invention, and Fig. 5 is a diagram showing the arrangement of the heating element and the detection body in an embodiment of the hot-wire pulse flowmeter of the present invention. FIG.

Claims (1)

【特許請求の範囲】 1 被測定流路内の被測定流体に対して所定の位
置において、瞬時的に前記被測定流体を加熱する
加熱手段と、 この加熱手段により加熱された前記被測定流体
の通過位置に設けられる感温素子と、 前記感温素子に接続され、加熱された被測定流
体が通過するのを検出する感温回路部と、 前記加熱手段による加熱から前記感温回路部の
検出までの時間を計測し、前記感温回路部の検出
から前記計測時間と等しい時間だけ更に経過後に
前記加熱手段を駆動する時間設定回路と、 この時間設定回路による加熱手段の駆動周期に
対応して前記被測定流体の流量を測定する手段
と、 前記被測定流体の流量が所定値以下になつたこ
とを検出するタイマー手段と、 そのタイマー手段の検出中、前記加熱手段を一
定周期で駆動するパルス発生器と、 を具備する熱線パルス流量計。
[Scope of Claims] 1. A heating means for instantaneously heating the fluid to be measured at a predetermined position with respect to the fluid to be measured in the flow path to be measured; a temperature sensing element provided at a passing position; a temperature sensing circuit unit connected to the temperature sensing element and detecting passage of the heated fluid to be measured; and detection of the temperature sensing circuit unit from heating by the heating means. a time setting circuit that measures the time from the temperature sensing circuit section and drives the heating means after a period of time equal to the measurement time has elapsed since the detection of the temperature sensing circuit section; means for measuring the flow rate of the fluid to be measured; timer means for detecting when the flow rate of the fluid to be measured falls below a predetermined value; and pulses for driving the heating means at a constant cycle while the timer means is detecting the flow rate of the fluid to be measured. A hot wire pulse flowmeter comprising: a generator;
JP56006836A 1981-01-19 1981-01-19 Heat ray pulse flowmeter Granted JPS57120816A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP56006836A JPS57120816A (en) 1981-01-19 1981-01-19 Heat ray pulse flowmeter
US06/422,975 US4483200A (en) 1981-01-19 1982-01-18 Thermal pulse flowmeter
PCT/JP1982/000017 WO1982002591A1 (en) 1981-01-19 1982-01-18 Heat-pulse type flow meter
DE19823231663 DE3231663C2 (en) 1981-01-19 1982-01-18 Measuring device for measuring the flow velocity and / or the flow volume of a fluid

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56006836A JPS57120816A (en) 1981-01-19 1981-01-19 Heat ray pulse flowmeter

Publications (2)

Publication Number Publication Date
JPS57120816A JPS57120816A (en) 1982-07-28
JPS6236523B2 true JPS6236523B2 (en) 1987-08-07

Family

ID=11649314

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56006836A Granted JPS57120816A (en) 1981-01-19 1981-01-19 Heat ray pulse flowmeter

Country Status (1)

Country Link
JP (1) JPS57120816A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2002088640A1 (en) * 2001-04-26 2002-11-07 Hiroyoshi Koizumi Method and equipment for measuring flow rate

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4542650A (en) * 1983-08-26 1985-09-24 Innovus Thermal mass flow meter
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DE2527378B2 (en) * 1975-06-19 1977-07-14 Bayer Ag, 5090 Leverkusen METHOD AND DEVICE FOR DOSING MULTI-COMPONENT LIQUID SYSTEMS

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WO2002088640A1 (en) * 2001-04-26 2002-11-07 Hiroyoshi Koizumi Method and equipment for measuring flow rate

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