Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS6257201B2 - - Google Patents
[go: Go Back, main page]

JPS6257201B2 - - Google Patents

Info

Publication number
JPS6257201B2
JPS6257201B2 JP56126971A JP12697181A JPS6257201B2 JP S6257201 B2 JPS6257201 B2 JP S6257201B2 JP 56126971 A JP56126971 A JP 56126971A JP 12697181 A JP12697181 A JP 12697181A JP S6257201 B2 JPS6257201 B2 JP S6257201B2
Authority
JP
Japan
Prior art keywords
signal
vortex
frequency
outputting
heat sensitive
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
JP56126971A
Other languages
Japanese (ja)
Other versions
JPS5827016A (en
Inventor
Shunichi Wada
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP56126971A priority Critical patent/JPS5827016A/en
Publication of JPS5827016A publication Critical patent/JPS5827016A/en
Publication of JPS6257201B2 publication Critical patent/JPS6257201B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Electrical Control Of Air Or Fuel Supplied To Internal-Combustion Engine (AREA)
  • Combined Controls Of Internal Combustion Engines (AREA)

Description

【発明の詳細な説明】 本発明は、自動車空気流量計測装置、特に渦流
量計の過渡特性の改良に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to improvements in the transient characteristics of automotive air flow measurement devices, particularly vortex flowmeters.

過流量計ではカルマン渦式のものと、スワール
式のものが、自動車用空気流量計として実用化さ
れており、ともに吸入空気量又は流速に略比例し
た周波数信号を出力する。
Karman vortex type and swirl type overflow meters have been put into practical use as air flow meters for automobiles, and both output frequency signals that are approximately proportional to the amount of intake air or flow velocity.

この周波数信号は広い流量範囲で精度が高く、
流速の過渡変化に対する追随性も非常に速いと云
う特長を持つ反面、周波数出力である為に渦の1
周期以上の高速応答は不可能であり特に低流量時
からの流速変化、大流量時からの急減速等での出
力の応答性が悪い欠点がある。さらに、周波数信
号の周期を計測して、より高速な空気流量計測を
行なおうとしても、渦のゆらぎにより生ずる周期
のゆらぎが存在する為、移動平均の様な平均化を
行なわないと安定な出力が望めず、さらに一層応
答性を損なうと云う欠点があつた。この欠点は、
吸入空気量をもとに自動車の燃料や排気ガスを制
御を行なう方式にとつては致命的である。
This frequency signal is highly accurate over a wide flow range.
It has the advantage of being very fast in following transient changes in flow velocity, but because it is a frequency output,
It is not possible to achieve a high-speed response that exceeds the period, and there is a drawback that the output response is poor, especially when the flow velocity changes from a low flow rate or when a sudden deceleration occurs from a high flow rate. Furthermore, even if you try to measure the period of the frequency signal to measure the air flow rate at a higher speed, there will be fluctuations in the period caused by fluctuations in the vortex, so it will not be stable unless averaging such as a moving average is performed. The disadvantage was that the output could not be expected and the response was further impaired. This drawback is
This is fatal for systems that control automobile fuel and exhaust gas based on the amount of intake air.

第1図に空気流量に比例した周波数出力を平均
化した場合の遅れの様子を示す。図中示したアナ
ログ空気流量の指示値に比べて、デイジタル化さ
れた周波数情報は次のパルスが入力されるまでは
古い情報を出力し続ける。この遅れ時間は最小の
時でもパルスの1周期分は必ず存在し、n個の平
均化を行なえばn個分必要である。
Figure 1 shows the delay when frequency output proportional to air flow rate is averaged. Compared to the analog air flow rate indication value shown in the figure, the digitized frequency information continues to output old information until the next pulse is input. This delay time always exists for one period of the pulse even when it is the minimum, and if n times are averaged, n times are required.

この平均化された周波数信号を用いて自動車の
燃料量を制御すれば加速時にはリーンに、減速時
にはリツチとなり好ましくない。逆に常に最小の
平均化時間で周波数出力を処理すれば、定常状態
での周波数のゆらぎが大きくなり問題である。
If the averaged frequency signal is used to control the amount of fuel in a car, it will become lean during acceleration and rich during deceleration, which is not desirable. On the other hand, if the frequency output is always processed using the minimum averaging time, frequency fluctuations in the steady state will become large, which is a problem.

この発明は上記欠点を除去する為のもので、渦
による周波数信号と同時に、流速に対応した電気
信号を出力する様にして周波数信号のもつ欠点を
解消しようとするものである。第2図は本発明の
一実施例の基本構成図である。
This invention is intended to eliminate the above-mentioned drawbacks, and aims to eliminate the drawbacks of the frequency signal by outputting an electrical signal corresponding to the flow velocity at the same time as the frequency signal caused by the vortex. FIG. 2 is a basic configuration diagram of an embodiment of the present invention.

第2図において1は吸入空気通路、2は渦発生
体、3,4は渦発生体2の後流に設けられた1対
の熱線である。熱線3は抵抗器5,6,7及び演
算増巾器11により、又熱線4は抵抗器8,9,
10及び演算増巾器12によりそれぞれ一定温度
に制御されている。この熱線3,4の制御電圧を
それぞれV1,V2とする。この制御電圧V1,V2
コンデンサ13,14,22、抵抗15,16,
17,18,20,21演算増巾器19よりなる
差信号増巾回路により、差の増巾信号V3とな
る。信号V3は波形整形回路23により周波数出
力V4つまり出力1となる。又、信号V1,V2は、
加算抵抗24,25,26により加算され、電圧
出力V5つまり出力2となる。
In FIG. 2, 1 is an intake air passage, 2 is a vortex generator, and 3 and 4 are a pair of hot wires provided downstream of the vortex generator 2. The hot wire 3 is connected to resistors 5, 6, 7 and the operational amplifier 11, and the hot wire 4 is connected to resistors 8, 9,
10 and an operational amplifier 12, each of which is controlled to a constant temperature. The control voltages of the hot wires 3 and 4 are assumed to be V 1 and V 2 , respectively. These control voltages V 1 and V 2 are connected to capacitors 13, 14, 22, resistors 15, 16,
17, 18, 20, 21 A difference signal amplification circuit comprising an operational amplifier 19 produces a difference amplification signal V3 . The signal V 3 becomes a frequency output V 4 , that is, an output 1, by the waveform shaping circuit 23 . Moreover, the signals V 1 and V 2 are
The voltages are added by adding resistors 24, 25, and 26 , resulting in a voltage output V5, that is, output 2.

第2図各部の電圧波形図を第3図に示す。第2
図の構成で渦発生体2の後流には左・右に対称で
規則的なカルマン渦列が発生する。熱線3,4は
平均流速により冷却されると同時に、カルマン渦
列により規則的にかつ交互に高い周波数で冷却さ
れる。この為、熱線3,4を一定温度に保つ為の
制御電圧V1,V2は、平均流速に対応した成分
及びカルマン渦による流速変化に対応成
分△V1,△V2とから成る。
FIG. 3 shows a voltage waveform diagram of each part in FIG. 2. Second
With the configuration shown in the figure, a regular Karman vortex street that is symmetrical to the left and right is generated in the wake of the vortex generator 2. The hot wires 3, 4 are cooled by the average flow velocity and at the same time regularly and alternately at a high frequency by the Karman vortex street. Therefore, the control voltages V 1 and V 2 for keeping the heating wires 3 and 4 at a constant temperature are components corresponding to the average flow velocity.
1 , 2 , and components △V 1 and △V 2 corresponding to changes in flow velocity due to Karman vortices.

この△V1と△V2は極性が反対であり、(△V1
△V2)×K1より信号V3が得られ、周波数出力V4
得られる。この周波数と吸入空気量との比率は略
一定である。
The polarities of △V 1 and △V 2 are opposite, and (△V 1
A signal V 3 is obtained from △V 2 )×K 1 , and a frequency output V 4 is obtained. The ratio between this frequency and the amount of intake air is approximately constant.

次に及びは、熱線と吸入空気温との間
の温度差が略一定であれば=(a+bU
〓)〓となり平均流速:Uの函数となる。信号
V1及び信号V2を加算する事により逆極性の△V1
と△V2とはキヤンセルされV5=K1(V1+V2)=
K2 =K2 (K1,K2は定数)となり、流速
Uの函数である信号V5が得られる。この信号V5
はアナログ電圧信号である為に応答性が良く、常
に流速Uに対応した情報を出力している。
Next, 1 and 2 are expressed as 1 = 2 = (a+bU
〓)〓 becomes the average flow velocity: a function of U. signal
By adding V 1 and signal V 2 , the opposite polarity △V 1
and △V 2 are canceled and V 5 = K 1 (V 1 + V 2 ) =
K 2 1 =K 2 2 (K 1 and K 2 are constants), and a signal V 5 which is a function of the flow velocity U is obtained. This signal V 5
Since it is an analog voltage signal, it has good responsiveness and always outputs information corresponding to the flow velocity U.

この信号V4及びV5を有効に並用する事により
高精度で高速応答の自動車用空気流量計が実現出
来る。
By effectively using signals V 4 and V 5 in parallel, a high-precision, high-speed response air flow meter for automobiles can be realized.

第2図において21はエンジンの運転状態を表
わす各種パラメータ情報でたとえばエンジンの回
転数情報、負圧、吸入空気温度、大気圧、水温等
である。必要に応じてこれらの情報を入力すれば
良い。22は空気流量信号処理回路である。
In FIG. 2, reference numeral 21 indicates various parameter information representing the operating state of the engine, such as engine rotational speed information, negative pressure, intake air temperature, atmospheric pressure, and water temperature. You can enter this information as necessary. 22 is an air flow signal processing circuit.

上記の様に構成された空気流量計において、吸
入空気量が急激に増加した場合を考える。V5
アナログ信号は吸入空気量に対応している為、
V5を微分すると吸入空気量の増加に対応した加
速信号が得られる。この加速信号に応じてV4
周波数信号の平均化の時間を変化させる様にすれ
ば、加速時にだけ平均化の時間を短かく応答遅れ
を小さく出来る。定常運転でV5のアナログ信号
の変化が小さい場合には長時間の平均化時間を確
保出来る。急激に減少した場合も同様である。こ
の場合には必要なエンジン運転パラメータとして
は吸入空気温度の情報だけで十分である。
Consider a case where the amount of intake air increases rapidly in the air flow meter configured as described above. Since the analog signal of V 5 corresponds to the amount of intake air,
By differentiating V5 , an acceleration signal corresponding to the increase in intake air amount can be obtained. By changing the averaging time of the frequency signal of V4 according to this acceleration signal, the averaging time can be shortened and the response delay can be reduced only during acceleration. If the change in the V5 analog signal is small during steady operation, a long averaging time can be secured. The same applies when there is a sudden decrease. In this case, information on the intake air temperature is sufficient as the necessary engine operating parameter.

なお上記実施例ではV5の微分信号によりV4
周波数信号の平均化の時間(又は移動平均の個
数)を変化させる場合について説明したが、平均
化の時間は必要なだけの長時間の固定にしておい
て、V5の微分信号の大きさに対応して増量係数
を決定して乗算する様にしても同様の効果が期待
出来る事は云うまでも無い。
In the above embodiment, the case where the averaging time (or the number of moving averages) of the frequency signal of V 4 is changed by the differential signal of V 5 was explained, but the averaging time may be fixed for as long as necessary. Needless to say, the same effect can be expected even if the increase coefficient is determined and multiplied according to the magnitude of the differential signal of V5 .

なお上記実施例ではカルマン渦列を1対の熱線
で検出する場合について述べたが、スワール式の
渦列の場合でも、同様の効果が期待出来る事は云
うまでもない。又渦の検出手段を熱線として述べ
たが、サーミスタその他の感熱素子であつても同
様の効果が期待出来る事は云うまでもない。
In the above embodiment, a case has been described in which the Karman vortex street is detected by a pair of hot wires, but it goes without saying that similar effects can be expected in the case of a swirl type vortex street. Furthermore, although the vortex detection means has been described as a heat wire, it goes without saying that similar effects can be expected even if a thermistor or other heat-sensitive element is used.

又、1対の熱線のうち片側の熱線が切れた場合
等で渦周波数の信号がもはや使用不可の様な場合
にも平均流速の信号をそのバツクアツプ信号とし
て用いる事が出来る。
Furthermore, even if the vortex frequency signal is no longer usable due to a break in one of the pair of heating wires, the average flow velocity signal can be used as a backup signal.

以上説明したとうり本発明によれば、周波数信
号の平均値に基づき、かつ、アナログ信号の変化
率に対応した空気流量信号を得る構成としたの
で、精度が高く応答性の優れた空気流量信号を得
ることができる効果がある。
As explained above, according to the present invention, since the air flow signal is obtained based on the average value of the frequency signal and corresponds to the rate of change of the analog signal, the air flow signal is highly accurate and has excellent responsiveness. There is an effect that can be obtained.

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

第1図は周波数出力信号を平均化した場合の欠
点を示すグラフ、第2図は本発明の一実施例の基
本構成図、第3図は第2図各部の電圧信号波形図
である。 図中1は吸入空気通路、2は渦発生体、3,4
は熱線である。V4は吸入空気量に略比例した周
波数出力信号、V5は吸入空気量に対応したアナ
ログ出力信号、21はエンジンの運転パラメータ
入力、22は空気流量信号処理回路である。
FIG. 1 is a graph showing the drawbacks when frequency output signals are averaged, FIG. 2 is a basic configuration diagram of an embodiment of the present invention, and FIG. 3 is a diagram of voltage signal waveforms at various parts in FIG. In the figure, 1 is the intake air passage, 2 is the vortex generator, 3, 4
is a hot ray. V 4 is a frequency output signal approximately proportional to the intake air amount, V 5 is an analog output signal corresponding to the intake air amount, 21 is an engine operating parameter input, and 22 is an air flow signal processing circuit.

Claims (1)

【特許請求の範囲】[Claims] 1 内燃機関の吸入空気通路に設けられ、下流に
渦を生じせしめる渦発生体の下流に設けられた一
対の感熱部を有し、これら一対の感熱部により第
1、第2の電気信号を得る感熱手段、この感熱手
段の上記第1、第2の電気信号の差に基づいて上
記渦の発生周期に対応した周波数信号を出力する
手段、上記第1、第2の電気信号の和に基づいて
平均流量に対応したアナログ信号を出力する手
段、及び上記周波数信号に基づいて演算し、所定
サンプリング個数の上記周波数信号の周期の平均
値または所定サンプリング時間内に発生する上記
周波数信号の周期の平均値に対応した所定の函数
となる空気流量信号を出力する信号処理手段と、
上記アナログ信号に基づいて上記信号処理手段の
上記サンプリング個数、上記サンプリング時間、
あるいは上記演算内容の少なくとも一つを制御す
る制御手段とを有する空気流量信号処理回路を備
え、空気流量の急変に対する応答性を向上せしめ
た機関の制御装置。
1. It has a pair of heat sensitive parts installed downstream of a vortex generator that is installed in the intake air passage of an internal combustion engine and generates a vortex downstream, and obtains first and second electrical signals by these pair of heat sensitive parts. a heat sensitive means, a means for outputting a frequency signal corresponding to the generation period of the vortex based on the difference between the first and second electric signals of the heat sensitive means, a means for outputting a frequency signal corresponding to the generation period of the vortex, based on the sum of the first and second electric signals; Means for outputting an analog signal corresponding to the average flow rate, and an average value of the periods of the frequency signals of a predetermined number of samples or an average value of the periods of the frequency signals occurring within a predetermined sampling time, calculated based on the frequency signals. signal processing means for outputting an air flow rate signal that is a predetermined function corresponding to;
the number of samplings of the signal processing means based on the analog signal, the sampling time;
Alternatively, an engine control device includes an air flow signal processing circuit having a control means for controlling at least one of the above calculation contents, and improves responsiveness to sudden changes in air flow.
JP56126971A 1981-08-11 1981-08-11 Device for controlling engine Granted JPS5827016A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56126971A JPS5827016A (en) 1981-08-11 1981-08-11 Device for controlling engine

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56126971A JPS5827016A (en) 1981-08-11 1981-08-11 Device for controlling engine

Publications (2)

Publication Number Publication Date
JPS5827016A JPS5827016A (en) 1983-02-17
JPS6257201B2 true JPS6257201B2 (en) 1987-11-30

Family

ID=14948420

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56126971A Granted JPS5827016A (en) 1981-08-11 1981-08-11 Device for controlling engine

Country Status (1)

Country Link
JP (1) JPS5827016A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59226239A (en) * 1983-06-06 1984-12-19 Nippon Denso Co Ltd Electronic fuel injection controlling apparatus for internal-combustion engine
JPS62174757U (en) * 1986-04-22 1987-11-06
JP5304766B2 (en) 2010-10-26 2013-10-02 株式会社デンソー Flow measuring device

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5924363A (en) * 1982-07-31 1984-02-08 Nec Home Electronics Ltd Common connecting system of bus for plural microcomputers

Also Published As

Publication number Publication date
JPS5827016A (en) 1983-02-17

Similar Documents

Publication Publication Date Title
EP1816445B1 (en) Thermal flow measuring device
US4872339A (en) Mass flow meter
JP3421245B2 (en) Heating resistor type air flow measurement device
US4457166A (en) Engine intake air flow measuring apparatus
JPS6257201B2 (en)
US4437345A (en) Gas flow measuring device
JP3470620B2 (en) Thermal air flow meter
JP2006138688A (en) Fluid flow meter and engine control system using the same
US4384484A (en) Gas flow measuring device
JPS5827015A (en) Airflow measuring device for automobile
JP3410562B2 (en) Temperature / wind speed measurement device
JP2004170357A (en) Exhaust gas flow rate measuring device and exhaust gas flow rate measuring method
JPH0835869A (en) Air flow meter
JP2533479B2 (en) Heating resistance type air flow meter
JPS595842A (en) Fuel controlling apparatus for internal combustion engine
JP3227084B2 (en) Air flow measurement device
JPH0235315A (en) hot wire air flow meter
JPS58110826A (en) Intake air temperature signal generating device for internal-combustion engine
JPS59136532A (en) Fuel control apparatus for internal-combustion engine
JPS6014908Y2 (en) Intake air amount detection device for internal combustion engine
JP2510151B2 (en) Thermal air flow measuring device for engine
JPS59136619A (en) Vortex flowmeter
JP2626628B2 (en) Heating resistance type air flow meter
JPH07166948A (en) Control device for internal combustion engine
JPH0143883B2 (en)