JPS5950939B2 - hot wire current meter - Google Patents

hot wire current meter

Info

Publication number
JPS5950939B2
JPS5950939B2 JP54128575A JP12857579A JPS5950939B2 JP S5950939 B2 JPS5950939 B2 JP S5950939B2 JP 54128575 A JP54128575 A JP 54128575A JP 12857579 A JP12857579 A JP 12857579A JP S5950939 B2 JPS5950939 B2 JP S5950939B2
Authority
JP
Japan
Prior art keywords
hot wire
wire
transistor
resistance
circuit
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
JP54128575A
Other languages
Japanese (ja)
Other versions
JPS5651670A (en
Inventor
博雅 久保
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.)
Nippon Denshi Kiki Co Ltd
Original Assignee
Nippon Denshi Kiki Co Ltd
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 Nippon Denshi Kiki Co Ltd filed Critical Nippon Denshi Kiki Co Ltd
Priority to JP54128575A priority Critical patent/JPS5950939B2/en
Publication of JPS5651670A publication Critical patent/JPS5651670A/en
Publication of JPS5950939B2 publication Critical patent/JPS5950939B2/en
Expired legal-status Critical Current

Links

Landscapes

  • Measuring Volume Flow (AREA)

Description

【発明の詳細な説明】 本発明は、流体中に配設された所定の金属線の抵抗温度
特性を利用して流速を測定する熱線式流速計に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a hot-wire anemometer that measures flow velocity using the resistance-temperature characteristics of a predetermined metal wire disposed in a fluid.

流体の流速を測定するための装置の一つに熱線式流速計
がある。
A hot wire anemometer is one of the devices for measuring the flow velocity of a fluid.

この流速計においては所定の抵抗温度特性を有する白金
等の金属線を熱線として流体中に配設しこの熱線が流体
の流速に応じた度合で冷却されて抵抗値が変化する性質
を利用している。このような熱線式流速計は金属線すな
わち熱線が流体に露出された構造であり、常に高速の流
体に接触しているさめ、正確な流速の測定及び熱線部分
の損傷等の防止するためには熱線部分は常に清浄に保ち
、熱容量と流体との摩擦抵抗の増加を防止する必要があ
る。
In this current meter, a metal wire such as platinum having a predetermined resistance temperature characteristic is placed in the fluid as a hot wire, and this hot wire is cooled to a degree according to the flow velocity of the fluid, making use of the property that the resistance value changes. There is. Hot wire anemometers have a structure in which a metal wire, i.e. a hot wire, is exposed to the fluid and is constantly in contact with high-speed fluid, so in order to accurately measure the flow velocity and prevent damage to the hot wire portion, it is necessary to It is necessary to keep the hot wire part clean at all times to prevent an increase in heat capacity and frictional resistance with the fluid.

特に、熱線式流速計を内燃機関の吸入空気流量の測定に
用いた場合、吸入空気中に塵埃が混入する率が高く、測
定毎に熱線に異物が付着するために経年変化を起し測定
値の信頼性が低下する。
In particular, when a hot-wire anemometer is used to measure the intake air flow rate of an internal combustion engine, the rate of dust contamination in the intake air is high, and foreign matter adheres to the hot wire each time the measurement is performed, causing deterioration over time and resulting in measured values. reliability decreases.

従つて測定終了時には熱線に付着した塵等異物を除去す
る必要がある。・ そこで従来から所定の金属線に大電
流を流し、これを高温にすることにより流体の流体測定
時に付着した塵等異物を焼切る熱線式流速計が考案され
ている。
Therefore, at the end of the measurement, it is necessary to remove foreign matter such as dust attached to the hot wire.・Therefore, a hot-wire anemometer has been devised in which a large current is passed through a predetermined metal wire to raise the temperature to a high temperature, thereby burning off foreign matter such as dust that adheres during fluid measurement.

以下、従来の熱線式流速計を第1図を参照して説明する
A conventional hot wire current meter will be explained below with reference to FIG.

第1図において熱線式流速計は熱線RHを一枝路に配置
し抵抗R、、R。
In Fig. 1, the hot wire current meter has a hot wire RH arranged in one branch and resistances R, , R.

、及びR。を残り三つの枝路に各々配置し上記熱線RH
に対向する枝路には抵抗R。と並列に抵抗R。とトラン
ジスタTlとからなるバイパス回路を有するブリッジ回
路と、上記トランジスタTiのベースに接続されトラン
ジスタTlを駆動するパルスを発生する駆動パルス発生
手段1と、上記ブロック回路の熱線RHを有する枝路と
熱線RHに相対し抵抗R、を有する枝路との接合点aを
熱線RHに対向し抵抗R。を有する枝路と抵抗R。に相
対し抵抗R。を有する枝路との接合点bとの間に所定圧
を供給する定電圧源VBと、更に、上記ブリッジ回路の
上記熱線RHを有する枝路と上記抵抗R。を有する枝路
との接合点cと上記抵抗R、を有する枝路と上記抵抗R
’を有する枝路との接合点dとに接続されかつ上記接合
点a ?、bとに接続され上記接合点cの電圧と上記接
合点dの電圧とを比較し定電圧源VBからブリッジ回路
内に流れる電流を制御する電流制御回路2とからなつて
いる。尚、上記電流制御回路2は演算増幅器OPとダー
リントン接続を構成しているトランジスタT。
, and R. are placed in each of the remaining three branches, and the above hot wire RH
There is a resistance R in the branch opposite to . resistor R in parallel with. and a transistor Tl, a drive pulse generating means 1 connected to the base of the transistor Ti and generating a pulse for driving the transistor Tl, and a branch circuit having a hot wire RH of the block circuit and a hot wire. The junction point a with the branch path which has a resistance R, which faces the hot wire RH, has a resistance R, which faces the hot wire RH. branch with resistance R. The resistance R is opposite to. a constant voltage source VB that supplies a predetermined voltage between a junction point b with the branch having the hot wire RH of the bridge circuit, and the resistor R and the branch having the hot wire RH of the bridge circuit. a junction point c with a branch path having a resistance R, and a branch path having a junction point c with the resistance R;
' and is connected to the junction point d with the branch road having the junction point a? , b, and compares the voltage at the junction point c with the voltage at the junction point d to control the current flowing from the constant voltage source VB into the bridge circuit. The current control circuit 2 includes a transistor T forming a Darlington connection with the operational amplifier OP.

とT。と更に抵抗R。とからなつており上記接合点cが
演算増幅器0Pの負入力端子に上記接合点dが正入力端
子に各々接続され演算増幅器0Pの出力がトランジスタ
T2のベースに接続されトランジスタT。のエミツタが
トランジスタT。のベースに接続されトランジスタT。
のコレクタがトランジスタT3のコレクタに接続されト
ランジスタT。のエミツタが抵抗R。を通してブリツジ
回路の上記接合点aに接続されトランジスタT。ののコ
レクタが上記接合点bに接続される。焼切り開始は流速
測定終了時の例えば内燃機関のイグニシヨンキ一がオフ
になり流体の流速が零になつた時点で行なうのが最も効
果的である。
and T. And further resistance R. The junction c is connected to the negative input terminal of the operational amplifier 0P, the junction d is connected to the positive input terminal, and the output of the operational amplifier 0P is connected to the base of the transistor T2. The emitter is a transistor T. connected to the base of the transistor T.
The collector of transistor T is connected to the collector of transistor T3. The emitter is resistance R. A transistor T is connected to the junction a of the bridge circuit through the transistor T. The collector of is connected to the junction b. It is most effective to start the burnout at the end of the flow velocity measurement, for example, when the ignition key of the internal combustion engine is turned off and the fluid flow velocity becomes zero.

これは熱の放散がないためである。上記タイミングにて
駆動パルス発生手段1から所定時間駆動パルスがトラン
ジスタT,に供給されるとトランジスタT,はオンにな
る。
This is because there is no heat dissipation. When a drive pulse is supplied from the drive pulse generating means 1 to the transistor T for a predetermined time at the above timing, the transistor T is turned on.

するとブリツジ回路の抵抗R。とバイパス回路の抵抗R
。とが並列合成されるためブリツジ回路の平衡が崩れ抵
抗R,とR。とR,とに大電流が流れる。電流制御回路
2では平衡時には所定電流が抵抗R,に流れていたが平
衡が崩れた時演算増幅器0Pの正入力端子側の方が負入
力端子側よりも高電位となるため出力が高電位となる。
このためトランジスタT。のコレクタ・エミツタ間電圧
VCEは大きくなり抵抗R。に流れる電流が減少し代つ
てブリツジ回路内に流れる電流が増加していく。従つて
熱線RHと抵抗R,とには大電流が流れそのため熱線R
Hの温度が急上昇し塵等付着していた異物は焼切れる。
そして熱線RHの温度が1,000℃を超えると熱線R
Hに付着していた塵等異物は完全に焼切れてしまうので
ある。ところが内燃機関のイグニシヨンキ一がオフにな
つた時その都度上記方法によつて焼切りを行なえば常に
熱線RHが1,000℃以上の温度に熱していることに
なる。
Then, the resistance R of the bridge circuit. and the resistance R of the bypass circuit
. Since these are combined in parallel, the balance of the bridge circuit collapses and the resistances R and R are combined in parallel. A large current flows through and R. In the current control circuit 2, a predetermined current flows through the resistor R when the balance is balanced, but when the balance is broken, the positive input terminal side of the operational amplifier 0P has a higher potential than the negative input terminal side, so the output becomes a high potential. Become.
For this reason, the transistor T. The collector-emitter voltage VCE increases and the resistance R increases. The current flowing in the bridge circuit decreases, and the current flowing in the bridge circuit increases. Therefore, a large current flows through the hot wire RH and the resistor R.
The temperature of H rises rapidly, and foreign matter such as dust is burned off.
When the temperature of the hot wire RH exceeds 1,000℃, the hot wire R
Any foreign matter such as dust attached to the H will be completely burned off. However, if the burnout is performed in accordance with the above method each time the ignition key of the internal combustion engine is turned off, the hot wire RH will always be heated to a temperature of 1,000° C. or more.

そのため熱線RHに用いた白金.線の表面が蒸発して行
き抵抗値の変化をきたし寿命もその回数分短かくなつて
いく。そこで本発明の目的は、上記した問題を解決した
長寿命の熱線式流速計を提供することにある。
Therefore, platinum was used for the hot wire RH. The surface of the wire evaporates, causing a change in resistance, and the lifespan of the wire is shortened by the number of times the wire evaporates. SUMMARY OF THE INVENTION An object of the present invention is to provide a long-life hot wire current meter that solves the above-mentioned problems.

上記目的を達成するため、内燃機関のイグニシ・ヨンキ
一がオフになる回数が自動車等車両の耐用年数からして
白金等の金属線を焼切りを行なう度に1,000℃程度
まで高温にすると抵抗値変化が許容値を超えることが多
いことを考慮して、焼切りを行なう時金属線に流す焼切
り電流パルスのうち少なくとも1つのパルス幅若しくは
ピーク値を大きくして金属線の塵等異物を焼切る温度を
約1,000℃と約800℃以下との2つに異ならしめ
るように構成されている。以下、本発明の実施例を第2
図を参照して説明する。
In order to achieve the above objective, the number of times the ignition switch of the internal combustion engine is turned off is increased to about 1,000 degrees Celsius each time metal wires such as platinum are burnt out, considering the service life of vehicles such as automobiles. Considering that the resistance value change often exceeds the allowable value, the pulse width or peak value of at least one of the burn-off current pulses applied to the metal wire is increased during burn-off to eliminate foreign matter such as dust on the metal wire. The structure is such that the temperature at which the material is burnt off is set to two different temperatures: about 1,000°C and about 800°C or less. Hereinafter, a second embodiment of the present invention will be described.
This will be explained with reference to the figures.

第2図において、本発明の回路構成はブリツジ回路と駆
動パルス発生手段1と電流制御回路2と′電源電圧供給
回路3とイグニシヨンキ一SWIとからなる。
In FIG. 2, the circuit configuration of the present invention includes a bridge circuit, a drive pulse generating means 1, a current control circuit 2, a power supply voltage supply circuit 3, and an ignition key SWI.

イグニシヨンキ一SW,はバツテリ等直流電源電圧VB
を点火装置5に供給している。尚、上記電流制御回路2
は第1図の場合と異なりブリツジ回路の熱線RHを有す
る枝路と抵抗R。を有する枝路との接合点Cにトランジ
スタT,のベースが接続されトランジスタT。のエミツ
タとトランジスタT5のベースとが接続されトランジス
タT。のエミツタと抵抗R。を通してブリツジ回路の熱
線RHを有する枝路と熱線RHに相対した抵抗R,を有
する枝路との接合点Aに接続されトランジスタT4のコ
レクタとトランジスタT5のコレクタとが共に接続され
てブリツジ回路の抵抗R2を有する枝路と抵抗R,を有
する枝路との接合点Bに接続されている。又、電源電圧
供給回路3は電源スイツチSW。
Ignition key SW, battery etc. DC power supply voltage VB
is supplied to the ignition device 5. In addition, the current control circuit 2
Unlike the case in FIG. 1, there is a branch circuit with a hot wire RH of the bridge circuit and a resistor R. The base of the transistor T is connected to the junction C with the branch having the transistor T. The emitter of the transistor T5 is connected to the base of the transistor T5. emitter and resistance R. is connected to the junction A of the branch with the hot wire RH of the bridge circuit and the branch with the resistor R opposite to the hot wire RH, through which the collectors of the transistor T4 and the collector of the transistor T5 are connected together, and the resistor of the bridge circuit is It is connected to the junction B of the branch with R2 and the branch with resistance R,. Further, the power supply voltage supply circuit 3 is a power switch SW.

と駆動信号発生手段4とからなつており、電源スイツチ
SW。の入力端子にバツテリ電源VBとイグニシヨンキ
一SW,とが接続され出力端子に上記ブリツジ回路の接
合点Aが接続され制御端子に駆動信号発生手段4が接続
され、そして駆動信号発生手段4の入力がイグニシヨン
キ一SW,と点火装置5との間に接続され、又、駆動パ
ルス発生手段1とも接続されている。流速測定時は電源
電圧供給回路3の電源スイツチSW。
and a drive signal generating means 4, including a power switch SW. The battery power supply VB and the ignition key SW are connected to the input terminal of the circuit, the junction point A of the bridge circuit is connected to the output terminal, the drive signal generation means 4 is connected to the control terminal, and the input of the drive signal generation means 4 is connected. It is connected between the ignition key SW and the ignition device 5, and is also connected to the drive pulse generating means 1. When measuring the flow velocity, use the power switch SW of the power supply voltage supply circuit 3.

を通して直流電源VBから熱線RHを含むブリツジ回路
の上記接合点AとBとの間に電圧が印加されている。ブ
リツジ回路に流れる電流は電流制御回路2にて制御され
ており、例えば接合点Cの電圧変化からブリツジ回路の
熱線RHの抵抗値変化を検出し流体の流速を算出してい
る。今、内燃機関のイグニシヨンキ一SW,がオフにな
つた時電源供給回路3の駆動信号発生手段4から駆動パ
ルス発生手段1に駆動信号が送られる。
A voltage is applied between the junction points A and B of the bridge circuit including the hot wire RH from the DC power source VB through the bridge circuit. The current flowing through the bridge circuit is controlled by a current control circuit 2, and the flow velocity of the fluid is calculated by detecting a change in the resistance value of the hot wire RH of the bridge circuit from a change in voltage at a junction point C, for example. Now, when the ignition key SW of the internal combustion engine is turned off, a drive signal is sent from the drive signal generation means 4 of the power supply circuit 3 to the drive pulse generation means 1.

駆動パルス発生手段1からイグニシヨンキ一SWlがオ
フになつた時点から所定時間T。
A predetermined time T has elapsed since the drive pulse generating means 1 turned off the ignition key SW1.

後パルス幅乙を有する駆動パルスがブリツジ回路の抵抗
R1を有する枝路と抵抗R2を有する枝路との接合点D
と上記接合点Bとの間に接続されたバイパス回路のトラ
ンジスタT1のベースに送られる。この時トランジスタ
T1はオン状態となり抵抗R2とR4とが並列合成され
る。するとブリツジ回路の平衡が崩れ抵抗R3に流れる
電流は一旦減少し電流制御回路2のトランジスタT4の
ベース電流が,減少する。これによりトランジスタT5
コレタタ・エミツタ問電圧。Eが増加しトランジスタT
5のコレクタ電流すなわち抵抗R6に流れる電流は減少
する。一方ブリツジ回路内には逆に直流電源VBからの
電流が増加し熱線RHが高温になり塵等異物が焼切れる
。この場合の焼切る温度は焼切れ電流を熱線RHに流す
時間に比例するので上記駆動パルスのパルス幅τを可変
することにより調節できる。例えば本発明の実施例によ
ると熱線に用いた白金を1,000℃迄上昇させ白金に
付着した塵等の異物を完全に焼切るのに必要なパルス幅
τは約1秒であつた。上記駆動パルス発生手段1は、熱
線RHの焼切り回数をカウントし所定回数カウントする
と、駆動パルスのパルス幅τを切替えて熱線RHを約1
,000℃に迄上昇させるに十分なパルス信号にし残り
の焼切り時には約800℃以下の適当な値に迄上昇させ
るパルス信号を発生するようにしている。
A driving pulse having a rear pulse width B is applied to a junction point D between a branch circuit having a resistance R1 and a branch circuit having a resistance R2 of the bridge circuit.
The signal is sent to the base of the transistor T1 of the bypass circuit connected between the junction point B and the junction point B. At this time, the transistor T1 is turned on and the resistors R2 and R4 are combined in parallel. Then, the balance of the bridge circuit collapses, the current flowing through the resistor R3 temporarily decreases, and the base current of the transistor T4 of the current control circuit 2 decreases. This causes transistor T5
Colletata emitsutata question voltage. E increases and transistor T
5, that is, the current flowing through the resistor R6 decreases. On the other hand, in the bridge circuit, the current from the DC power supply VB increases, and the hot wire RH becomes high in temperature, thereby burning off foreign matter such as dust. Since the burnout temperature in this case is proportional to the time during which the burnout current is passed through the hot wire RH, it can be adjusted by varying the pulse width τ of the drive pulse. For example, according to an example of the present invention, the pulse width τ required to raise the platinum used in the hot wire to 1,000° C. and completely burn off foreign matter such as dust attached to the platinum was about 1 second. The drive pulse generating means 1 counts the number of times the hot wire RH is burnt out, and when it has counted a predetermined number of times, it switches the pulse width τ of the drive pulse to reduce the heat wire RH by approximately 1.
The pulse signal is sufficient to raise the temperature up to ,000°C, and during the remaining burnout, a pulse signal is generated to raise the temperature to an appropriate value of about 800°C or less.

そのために例えばカウンタとワンシヨツトマルチとが用
いられている。尚、上記熱線の焼切り実施後駆動パルス
発生手段1から終了を示す信号が電源電圧供給回路3の
駆動信号発生手段4に送られる。
For this purpose, counters and one-shot multis are used, for example. After the hot wire is burnt out, a signal indicating the completion is sent from the drive pulse generation means 1 to the drive signal generation means 4 of the power supply voltage supply circuit 3.

駆動信号発生手段4では上記信号を受取ると電源スイツ
チSW2の制御端子に送つていた信号を切り電源スイツ
チSW2をオフにしている。又、他の実施例としてブリ
ツジ回路の抵抗R4とトランジスタT1とからなるバイ
パス回路においてトランジスタT1のベースに入る駆動
パルス幅を所定値にしておき抵抗R4の値を切替えるこ
とにより熱線RHに流れる焼切り電流値を異ならしめる
構成としても熱線に流れる電流値に比例して熱線の温度
が上昇するという特性からして同様な効果をもたらすも
のである。
When the drive signal generating means 4 receives the above signal, it cuts off the signal sent to the control terminal of the power switch SW2, thereby turning off the power switch SW2. As another example, in a bypass circuit consisting of a resistor R4 of a bridge circuit and a transistor T1, the width of the driving pulse applied to the base of the transistor T1 is set to a predetermined value, and the value of the resistor R4 is changed to reduce the burnout flowing to the hot wire RH. Even a configuration in which the current values are made different can bring about the same effect because of the characteristic that the temperature of the hot wire rises in proportion to the value of the current flowing through the hot wire.

以上の様に、熱線式流速計の熱線の焼切る温度を焼切る
回数のうち所定回数のうち1度は1,000℃程度の高
温にし他の焼切り時には上記温度より低い適当な値にす
ることにより熱線に付着した塵等異物は完全に除去でき
しかも熱線の焼切りによる抵抗値変化を出来るだけ低く
抑えることができる。
As mentioned above, the temperature at which the hot wire of the hot wire type anemometer burns out is set to a high temperature of about 1,000 degrees Celsius for one predetermined number of burnouts, and is set to an appropriate value lower than the above temperature for other burnouts. As a result, foreign matter such as dust attached to the hot wire can be completely removed, and changes in resistance value due to burning out of the hot wire can be suppressed as low as possible.

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

第1図は従来の熱線式流速計を示し、第2図は本発明の
熱線式流速計の一実施例を示す。 主要部分の符号の説明、RH・・・・・・熱線、T1〜
T5・・・・・・トランジスタ、0P・・・・・・演算
増幅器、SWl・・・・・・イグニシヨンキ一、R1〜
R2・・・・・・抵抗、SW2・・・・・・電源スイツ
チ、A,B,C,D,a,b,c,d・・・・・・接合
点、1・・・・・・駆動パルス発生手段、2・・・・・
・電流制御回路、3・・・・・・電源電圧供給回路、4
・・・”・・・駆動信号発生手段、5・・・・・・点火
装置、8・・・・・・直流電源。
FIG. 1 shows a conventional hot-wire type current meter, and FIG. 2 shows an embodiment of the hot-wire type current meter of the present invention. Explanation of symbols of main parts, RH...Heat wire, T1~
T5...Transistor, 0P...Operation amplifier, SWl...Ignition key, R1~
R2... Resistor, SW2... Power switch, A, B, C, D, a, b, c, d... Junction, 1... Drive pulse generating means, 2...
・Current control circuit, 3... Power supply voltage supply circuit, 4
..."... Drive signal generating means, 5... Ignition device, 8... DC power supply.

Claims (1)

【特許請求の範囲】[Claims] 1 流体の通路に配設された所定の抵抗温度特性を有す
る金属線と、前記金属線に接続され両端に所定電圧を供
給する定電圧源と、内燃機関のイグニシヨンキーがオフ
の時に前記金属線に焼切り電流パルスを供給する金属線
焼切り電流パルス発生手段とからなる熱線式流速計であ
つて、N(N≧2)個発生する前記焼切り電流パルスの
うち少なくとも1つのパルス幅若しくはピーク値が他の
パルス幅若しくはピーク値とは大なることを特徴とする
もの。
1. A metal wire having a predetermined resistance-temperature characteristic disposed in a fluid passage, a constant voltage source connected to the metal wire and supplying a predetermined voltage to both ends, and A hot wire anemometer comprising a metal wire burnout current pulse generating means for supplying a burnout current pulse to the wire, wherein at least one of the N (N≧2) generated burnout current pulses has a pulse width or A device characterized in that its peak value is larger than other pulse widths or peak values.
JP54128575A 1979-10-04 1979-10-04 hot wire current meter Expired JPS5950939B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP54128575A JPS5950939B2 (en) 1979-10-04 1979-10-04 hot wire current meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP54128575A JPS5950939B2 (en) 1979-10-04 1979-10-04 hot wire current meter

Publications (2)

Publication Number Publication Date
JPS5651670A JPS5651670A (en) 1981-05-09
JPS5950939B2 true JPS5950939B2 (en) 1984-12-11

Family

ID=14988137

Family Applications (1)

Application Number Title Priority Date Filing Date
JP54128575A Expired JPS5950939B2 (en) 1979-10-04 1979-10-04 hot wire current meter

Country Status (1)

Country Link
JP (1) JPS5950939B2 (en)

Also Published As

Publication number Publication date
JPS5651670A (en) 1981-05-09

Similar Documents

Publication Publication Date Title
US4210016A (en) Flow rate meter with temperature-dependent resistor
JPS61198023A (en) Measuring device of quantity of air
JPS63134920A (en) Flow measuring device
US4450719A (en) Air flow meter
JPS6260650B2 (en)
JPH0216453B2 (en)
JP3969167B2 (en) Fluid flow measuring device
GB2064784A (en) Device for measuring the mass of a flowing medium
JPH0422206B2 (en)
JPS5950939B2 (en) hot wire current meter
JPH09500969A (en) Method and circuit arrangement for protecting a temperature-dependent heated sensor resistance from overheating
JPH03120423A (en) Method and apparatus for controlling temperature of measuring resistor
JPS6039542A (en) Smoke density detecting method
US4571991A (en) Air flow measuring apparatus
JPS62280615A (en) Sticking matter burning-off circuit for hot-wire type air flow meter
JPS61715A (en) Thermal air-flow detector
JPH0518665Y2 (en)
JPS5942699Y2 (en) Power control circuit for hot wire current meter
JPH0357413B2 (en)
JPH04501154A (en) resistance temperature control device
JPH02653Y2 (en)
JPH0448221A (en) Air suction amount detector
SU821952A2 (en) Temperature measuring device
JPS6334309B2 (en)
JP3184402B2 (en) Thermal air flow detector