JPS6355358A - Drive circuit of fuel atomizer for internal combustion engine - Google Patents

Drive circuit of fuel atomizer for internal combustion engine

Info

Publication number
JPS6355358A
JPS6355358A JP19888986A JP19888986A JPS6355358A JP S6355358 A JPS6355358 A JP S6355358A JP 19888986 A JP19888986 A JP 19888986A JP 19888986 A JP19888986 A JP 19888986A JP S6355358 A JPS6355358 A JP S6355358A
Authority
JP
Japan
Prior art keywords
frequency
voltage
circuit
oscillation
current
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.)
Pending
Application number
JP19888986A
Other languages
Japanese (ja)
Inventor
Hiroshi Koike
博 小池
Hiroshi Yoneda
浩志 米田
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.)
Hitachi Ltd
Hitachi Automotive Systems Engineering Co Ltd
Original Assignee
Hitachi Automotive Engineering Co Ltd
Hitachi 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 Hitachi Automotive Engineering Co Ltd, Hitachi Ltd filed Critical Hitachi Automotive Engineering Co Ltd
Priority to JP19888986A priority Critical patent/JPS6355358A/en
Publication of JPS6355358A publication Critical patent/JPS6355358A/en
Pending legal-status Critical Current

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  • Apparatuses For Generation Of Mechanical Vibrations (AREA)

Abstract

PURPOSE:To improve the efficiency, by feedback controlling an exciting frequency such that the current flowing through a high voltage generating coil for applying voltage across a supersonic vibration chip and atomizing fuel is maximized, thereby exciting a supersonic vibration chip near a resonant point. CONSTITUTION:An A.C. voltage is applied across a piezoelectric element in a supersonic vibration chip 1 so as to cause supersonic vibration thereof thus atomizing fuel. A high voltage generating coil 2 for applying a high A.C. voltage across said supersonic vibration chip 1 is fed with power from a power source 3 so as to produce a high voltage corresponding to a winding ratio of secondary winding through primary winding current being interrupted alternately by power transistors 4, 5. The oscillation frequency of an oscillation circuit 100 for interrupting the power transistors 4, 5 alternately is feedback controlled so that the driving current flowing through the emitters of the power transistors 4, 5 is maximized.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は内燃機関の燃料通路に設けられた超音波振動子
により燃料を微粒化する内燃機関用燃料微粒化装置の駆
動回路に係り、特に超音波振動子の励振周波数を振動子
の共振点付近に自動制御して最大出力を安定にえられる
内燃機関用燃料微粒化装置の駆動回路に関する。
[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a drive circuit for a fuel atomization device for an internal combustion engine that atomizes fuel using an ultrasonic vibrator provided in a fuel passage of the internal combustion engine, and particularly The present invention relates to a drive circuit for a fuel atomization device for an internal combustion engine that can stably obtain maximum output by automatically controlling the excitation frequency of an ultrasonic vibrator to near the resonance point of the vibrator.

〔従来の技術〕[Conventional technology]

従来の超音波振動子による内燃機関用燃料微粒化装置の
駆動回路としては、たとえば特開昭58−210354
号公報に記載のように超音波振動子の励振周波数を共振
点付近で所定の周期で変化させる回路が知られている。
As a drive circuit for a fuel atomization device for an internal combustion engine using a conventional ultrasonic vibrator, for example, Japanese Patent Application Laid-Open No. 58-210354
As described in the above publication, a circuit is known that changes the excitation frequency of an ultrasonic transducer at a predetermined period near a resonance point.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

上記従来技術は超音波振動子の共振点付近で所定の周期
と幅で励振周波数を上下させる方式であるため、その励
振周波数が共振点にある時間は全体の何分の1かになっ
て効率が低下するという問題点が卆った。
The above conventional technology is a method of raising and lowering the excitation frequency at a predetermined period and width near the resonance point of the ultrasonic transducer, so the time that the excitation frequency is at the resonance point is a fraction of the total, resulting in efficiency. A problem arose in that the value decreased.

本発明の目的は超音波振動子の励振周波数を共振点付近
に自動制御して最大出力を安定にえられる内燃機関用燃
料微粒化装置の駆動回路を提供するにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a drive circuit for a fuel atomization device for an internal combustion engine that can automatically control the excitation frequency of an ultrasonic vibrator to near the resonance point to stably obtain maximum output.

〔問題点を解決するための手段〕  −上記目的は、超
音波振動子の駆動電流を検出し、共振点付近で駆動電流
が急上昇する領域において駆動電流が一定になるように
超音波振動子の励振周波数をフィードバック制御する手
段を備えた内燃機関用燃料微粒化装置の駆動回路により
達成される。
[Means for solving the problem] - The above purpose is to detect the drive current of the ultrasonic transducer and adjust the drive current of the ultrasonic transducer so that the drive current becomes constant in the region where the drive current rapidly increases near the resonance point. This is achieved by a drive circuit for a fuel atomizer for an internal combustion engine that is equipped with means for feedback controlling the excitation frequency.

〔作用〕[Effect]

上記手段による内燃機関用燃料微粒化装置の駆動回路で
は、超音波振動子の共振点付近で駆動回路からの駆動電
流が急増するのを検出して超音波振動子の励振周波数を
制御しているので、その励振周波数を共振点付近に安定
して追随させることができる。
In the drive circuit of the fuel atomization device for an internal combustion engine according to the above means, the excitation frequency of the ultrasonic vibrator is controlled by detecting a sudden increase in the drive current from the drive circuit near the resonance point of the ultrasonic vibrator. Therefore, the excitation frequency can be stably tracked near the resonance point.

〔実施例〕〔Example〕

以下に本発明の一実施例を第1図ないし第5図により説
明する。
An embodiment of the present invention will be described below with reference to FIGS. 1 to 5.

第1図は本発明による内燃機関用燃料微粒化装置の駆動
回路の一実施例を示す全体構成図である。
FIG. 1 is an overall configuration diagram showing one embodiment of a drive circuit of a fuel atomization device for an internal combustion engine according to the present invention.

第1図において、1は超音波振動子で内燃機関の燃料通
路の途中に設けられ、その圧電素子に加えられる交流電
圧により超音波振動して内燃機関の燃料を微粒化する。
In FIG. 1, an ultrasonic vibrator 1 is installed in the middle of a fuel passage of an internal combustion engine, and is vibrated ultrasonically by an alternating current voltage applied to the piezoelectric element to atomize the fuel of the internal combustion engine.

2は高電圧発生用コイルでセンタータップをもつ1次巻
線と2次巻線と鉄心とからなり、3は電源、4,5はパ
ワートランジスタで、高電圧発生用コイル2は電源3か
ら電力供給されパワートランジスタ4.5により交互に
通流遮断する1次巻線電流により、2次巻線に巻数比に
応じた高圧交流電圧を発生させて上記超音波周波数1に
印加する。
2 is a high voltage generation coil that consists of a primary winding with a center tap, a secondary winding, and an iron core; 3 is a power supply; 4 and 5 are power transistors; high voltage generation coil 2 receives power from power supply 3; The supplied primary winding current, which is alternately turned on and off by the power transistor 4.5, generates a high-voltage AC voltage in the secondary winding according to the turns ratio and is applied at the ultrasonic frequency 1.

また100は発振回路で超音波周波数たとえば28 k
 Hz〜40kHz程度の周波数の発振を行ない、パワ
ートランジスタ4,5を交互に逆流遮断するベース電流
を供給する。200は周波数制御回路で発振回路100
の発振周波数を制御して電流検出回路の出力により発振
周波数を変化させる。300は電流検出回路でパワート
ランジスタ4.5のエミッタに流れる駆動電流により高
電圧発生用コイル2の電流を検出し、その出力により周
波数制御回路200の動作を制御する。
In addition, 100 is an oscillation circuit with an ultrasonic frequency of, for example, 28 k.
It oscillates at a frequency of about Hz to 40 kHz and supplies a base current that alternately blocks the reverse flow of the power transistors 4 and 5. 200 is a frequency control circuit and an oscillation circuit 100
The oscillation frequency is controlled and the oscillation frequency is changed by the output of the current detection circuit. Reference numeral 300 denotes a current detection circuit which detects the current of the high voltage generation coil 2 by the drive current flowing to the emitter of the power transistor 4.5, and controls the operation of the frequency control circuit 200 by its output.

第2図は第1図の超音波振動子1の出力特性図である。FIG. 2 is an output characteristic diagram of the ultrasonic transducer 1 shown in FIG. 1.

第2図において、超音波振動子1の出力は励振周波数が
振動子の共振点付近で急上昇して共振点と一致するとき
に最大値となり、共振点から離れるほど出力が低下する
。また超音波振動子1の出力の変化は高電圧発生用コイ
ル2の入力の変化と相対的に一致するから、パワートラ
ンジスタ4,5に流れる電流すなわち高電圧発生用コイ
ル2の電流も振動子1の共振点付近で急上昇して共振点
で最大となる。
In FIG. 2, the output of the ultrasonic transducer 1 reaches its maximum value when the excitation frequency rapidly increases near the resonance point of the transducer and coincides with the resonance point, and the output decreases as the distance from the resonance point increases. Furthermore, since the change in the output of the ultrasonic transducer 1 is relatively consistent with the change in the input to the high voltage generation coil 2, the current flowing through the power transistors 4 and 5, that is, the current in the high voltage generation coil 2, also changes to the transducer 1. It rises rapidly near the resonance point and reaches its maximum at the resonance point.

上記構成による第1図の駆動回路の動作を説明すると、
まず発振回路100の発振周波数は周波数制御回路20
0の出力により例えば振動手1の共振点より高いある所
定の周波数で発振し、その周波数から徐々に下降するよ
うに変化する。するとこの発振周波数が振動子1の共振
周波数に近付くにつれ、高電圧発生コイル2の電流は急
上昇する。この高電圧発生コイル2の電藻を電流検出口
1300によりパワートランジスタ5.6のエミッタに
流れる駆IjJ電流として検出し、この検出電流値が設
定値に達したならば周波数制御回路200に出力信号を
送って上記発振回路100の発揚周波数の下降を停止さ
せるようにフィードバックをかける。このフィードバッ
ク量を適当に選ぶことにより、発振周波数を振動子1の
共振点付近のある設定値に固定できる。
The operation of the drive circuit shown in FIG. 1 with the above configuration will be explained as follows.
First, the oscillation frequency of the oscillation circuit 100 is determined by the frequency control circuit 20.
With an output of 0, for example, the vibrating hand 1 oscillates at a certain predetermined frequency higher than its resonance point, and gradually decreases from that frequency. Then, as this oscillation frequency approaches the resonant frequency of the vibrator 1, the current in the high voltage generating coil 2 increases rapidly. The current of this high voltage generating coil 2 is detected by the current detection port 1300 as a driving IjJ current flowing to the emitter of the power transistor 5.6, and when this detected current value reaches a set value, an output signal is sent to the frequency control circuit 200. is sent to apply feedback to stop the drop in the oscillation frequency of the oscillation circuit 100. By appropriately selecting this amount of feedback, the oscillation frequency can be fixed at a certain set value near the resonance point of the vibrator 1.

このようにして超音波振動子1の共振点より少し高い発
振周波漱で振動子1を安定に励振でき、かつi動子1の
套振周波数が変化した場合にも自動的に追随゛してその
共振点付近で安定する。なお発振回路10”Oの発振周
波数を振動子1の共振点より低い周波数から徐々に上昇
するように変化させると、同様の制御動作により共振点
より少し低い発振周波数で安定する。
In this way, it is possible to stably excite the transducer 1 at an oscillation frequency slightly higher than the resonance point of the ultrasonic transducer 1, and it can also automatically follow changes in the vibration frequency of the i-oscillator 1. It becomes stable near its resonance point. Note that when the oscillation frequency of the oscillation circuit 10''O is changed to gradually increase from a frequency lower than the resonance point of the vibrator 1, the oscillation frequency is stabilized at a slightly lower frequency than the resonance point by a similar control operation.

つぎに第3図は楢1図の発振回路IC)Oの一実施例を
示す回路図である。第3図において、発振回路100と
しては例えば電圧制御発振回路が使用できる。101,
102,103.i04は抵抗器、105はコンデンサ
、106は演算増幅器、ro7.16’s、’ 109
,110.t 11は抵抗器、112は比較器、113
.i14,115は抵抗器、116は比較器で、これら
により電圧制御発振器を構成する。117はトランジス
タ。
Next, FIG. 3 is a circuit diagram showing an embodiment of the oscillation circuit IC)O shown in FIG. In FIG. 3, for example, a voltage controlled oscillation circuit can be used as the oscillation circuit 100. 101,
102, 103. i04 is a resistor, 105 is a capacitor, 106 is an operational amplifier, ro7.16's,' 109
, 110. t 11 is a resistor, 112 is a comparator, 113
.. I14 and 115 are resistors, and 116 is a comparator, which constitute a voltage controlled oscillator. 117 is a transistor.

118は抵抗器、119はトランジスタ、120゜12
1は抵抗器、122はトランジスタ、123は抵抗器、
124はトランジスタ、125は抵抗器である。
118 is a resistor, 119 is a transistor, 120°12
1 is a resistor, 122 is a transistor, 123 is a resistor,
124 is a transistor, and 125 is a resistor.

上記構成による発振回路100の電圧制御発振器は公知
であるから詳細動作説明を省略するが。
Since the voltage controlled oscillator of the oscillation circuit 100 having the above configuration is well known, a detailed explanation of its operation will be omitted.

抵抗器101,102の接続点の入力電圧v1により発
振周波数の変化する矩形波電圧が比較器112の出力に
発生する。トランジスタ117はエミッタフォロワー回
路を形成しており、エミッタに接続される抵抗器118
,121の値により比較器112の出力電圧が変化して
発振周波数が変化するのを防止する。トランジスタ11
9は発振出力を増幅してパワートランジスタ4を駆動し
、トランジスタ122,124はパワートランジスタ4
と位相を反転させた発振出力でパワートランジスタ5を
駆動する。
A rectangular wave voltage whose oscillation frequency changes is generated at the output of the comparator 112 according to the input voltage v1 at the connection point of the resistors 101 and 102. The transistor 117 forms an emitter follower circuit, and the resistor 118 is connected to the emitter.
, 121 prevents the output voltage of the comparator 112 from changing and the oscillation frequency from changing. transistor 11
9 amplifies the oscillation output to drive the power transistor 4; transistors 122 and 124 drive the power transistor 4;
The power transistor 5 is driven by an oscillation output whose phase is inverted.

このようにして発振回路100は周波数制御回路200
からの入力電圧Vl により決まる発振周波数で位相が
反転した2個の矩形波電圧を発生して、パワートランジ
スタ4,5を駆動する。
In this way, the oscillation circuit 100 is controlled by the frequency control circuit 200.
The power transistors 4 and 5 are driven by generating two rectangular wave voltages whose phases are inverted at an oscillation frequency determined by the input voltage Vl from the input voltage Vl.

第4図は第1図の周波数制御回路200の一実施例を示
す回路図である。第4図において、201゜202は抵
抗器で電圧Vccを分割して発振回路100の発振周波
数を決める電圧Vl の最大値を決める。203,20
4は抵抗器、205はトランジスタ、206は抵抗器、
207はトランジスタで定電流回路を構成しており、2
08はコンデンサで上記定電流回路により充電してコン
デンサ208のA点電圧を下降させる。209は演算増
幅器で出力を負入力に帰還して出力電圧v1の値による
コンデンサ208の電圧上昇変化がないようにインピー
ダンス変換する。210はダイオードで出力電圧Vl側
からコンデンサ208側へのみ電流を供給して逆方向に
は流さないようにする。
FIG. 4 is a circuit diagram showing an embodiment of the frequency control circuit 200 of FIG. 1. In FIG. 4, resistors 201 and 202 divide the voltage Vcc to determine the maximum value of the voltage Vl that determines the oscillation frequency of the oscillation circuit 100. In FIG. 203,20
4 is a resistor, 205 is a transistor, 206 is a resistor,
207 constitutes a constant current circuit with a transistor;
A capacitor 08 is charged by the constant current circuit to lower the voltage at point A of the capacitor 208. Reference numeral 209 is an operational amplifier which feeds back the output to the negative input and converts the impedance so that there is no change in voltage increase of the capacitor 208 due to the value of the output voltage v1. A diode 210 supplies current only from the output voltage Vl side to the capacitor 208 side and prevents it from flowing in the opposite direction.

211は抵抗f、+、212はトランジスタで電流検出
回路300の出力によりコンデンサ208を放電して充
1ffi圧を下げ、コンデンサ208のA点電圧を上げ
る働きをする。
211 is a resistor f, +; 212 is a transistor that discharges the capacitor 208 by the output of the current detection circuit 300, lowers the charging 1ffi pressure, and increases the A point voltage of the capacitor 208;

上記構成による周波数制御回路において、コンデンサ2
08のA点電圧とダイオード210の電圧ドロップとの
和が抵抗器201と抵抗器202の分割電圧より高パう
ちは・発振回路100の空振周波数を決めるt圧Vl 
は電圧Vccを抵抗器201.202により分割した値
で決まる。ついでコンデンサ208が定電流によって充
電されてA点電圧とダイオード210の電圧ドロップと
の和が上記分割電圧より低くなると、電圧V、はコンデ
ンサ208のA点電圧で決まるようになる。
In the frequency control circuit with the above configuration, capacitor 2
The sum of the A point voltage of 08 and the voltage drop of the diode 210 is higher than the divided voltage of the resistor 201 and the resistor 202. t pressure Vl that determines the air vibration frequency of the oscillation circuit 100
is determined by the value obtained by dividing the voltage Vcc by resistors 201 and 202. Then, when the capacitor 208 is charged with a constant current and the sum of the voltage at the point A and the voltage drop of the diode 210 becomes lower than the divided voltage, the voltage V is determined by the voltage at the point A of the capacitor 208.

さらに発振回路100により駆動されるパワートランジ
スタ4,5の電流により出力側からフィードバックがか
かつて電流検出回路300からの出力信号によりトラン
ジスタ212がオンすると、その゛出力信号の幅と抵抗
器211およびコンデンサ208の容量による時定数と
で決まる電圧分だけコンデンサ208の電圧が下がって
A点電圧1上上がる。
Furthermore, when feedback is generated from the output side by the currents of the power transistors 4 and 5 driven by the oscillation circuit 100 and the transistor 212 is turned on by the output signal from the current detection circuit 300, the width of the output signal and the resistor 211 and capacitor are The voltage of the capacitor 208 decreases by a voltage determined by the time constant due to the capacitance of the capacitor 208, and the voltage at the point A increases by 1.

こうして発振回路100の発振周波数を決定する周波数
制御回路300の出力電圧Viは当初の抵抗器201,
202の分割比で決まる電圧Vccの分割電圧からスタ
ートし、ついでコンデンサ208が充電されてコンデン
サ208のA点電圧とダイオード210の電圧ドロップ
との和が上記分割電圧以下になるとA点電圧に伴って徐
々に下降する。さらに出力側からフィードバックがかか
つて電流検出回路300からの出力信号が入ると電圧V
、は一時的に上昇して、電流検出回路300の出力がな
くなると再び下降するように制御され、発振回路100
の発振周波数を所定値に自動制御する。
In this way, the output voltage Vi of the frequency control circuit 300 that determines the oscillation frequency of the oscillation circuit 100 is
The capacitor 208 is charged, and when the sum of the A-point voltage of the capacitor 208 and the voltage drop of the diode 210 becomes less than the above-mentioned divided voltage, the A-point voltage increases. Gradually descend. Furthermore, when feedback is applied from the output side and the output signal from the current detection circuit 300 is input, the voltage V
, is controlled to rise temporarily and fall again when the output of the current detection circuit 300 disappears, and the oscillation circuit 100
automatically controls the oscillation frequency to a predetermined value.

第5図は第1図の電流検出回路300の一実施例を示す
回路図である。第5図において、301は抵抗器でパワ
ートランジスタ4,5からの電流を検出する。302は
コンデンサで抵抗器301の電圧ドロップを平滑する。
FIG. 5 is a circuit diagram showing an embodiment of the current detection circuit 300 of FIG. 1. In FIG. 5, 301 is a resistor that detects the current from the power transistors 4 and 5. A capacitor 302 smoothes the voltage drop of the resistor 301.

303はコンパレータ、304,305は抵抗器でコン
パレータ303の基や1を圧を決める。306は抵抗器
でコンパレ−夕303の出力を周波数制御回路200へ
伝える。
303 is a comparator, and 304 and 305 are resistors that determine the pressure of the comparator 303 and 1. A resistor 306 transmits the output of the comparator 303 to the frequency control circuit 200.

上記構成による電流検出回路300において、パワート
ランジスタ4,5のエミッタに流れる電流は抵抗器30
1により検出され、この電流値による電圧ドロップ値が
分割抵抗器304,305で設定された基準電圧値以上
になると、コンパレータ303から出力信号が周波数制
御回路200に対して送られる。
In the current detection circuit 300 with the above configuration, the current flowing through the emitters of the power transistors 4 and 5 is connected to the resistor 30.
1, and when the voltage drop value due to this current value exceeds the reference voltage value set by the dividing resistors 304 and 305, an output signal is sent from the comparator 303 to the frequency control circuit 200.

上記実施例によれば、超音波振動子による内燃機関用燃
料微粒化装置の駆動回路において振動子の励振周波数が
共振点付近にないと所要の振動振幅かえられず、これに
対して振動子の共振点が振動子への燃料の付着や温度特
性によって変化するため固定周波数では有効に機能しな
いが、振動子の共振点付近では駆動電流が急増するのを
高電圧発生用コイル電流を通流遮断するパワートランジ
スタの電流により検出してフィードバックをかけて自動
制御することにより常に安定して共振点付近で振動子を
励振させることが可能であり、なお発振回路の発振周波
数が温度によって変動するのも補償される。
According to the above embodiment, in the drive circuit of a fuel atomization device for an internal combustion engine using an ultrasonic vibrator, if the excitation frequency of the vibrator is not near the resonance point, the required vibration amplitude cannot be changed; It does not work effectively at a fixed frequency because the point changes depending on the adhesion of fuel to the vibrator and temperature characteristics, but the high voltage generation coil current is cut off to prevent the drive current from increasing rapidly near the vibrator's resonance point. By detecting the current of the power transistor and applying feedback for automatic control, it is possible to always stably excite the resonator near the resonance point, and it is also possible to compensate for fluctuations in the oscillation frequency of the oscillation circuit due to temperature. be done.

〔発明の効果〕〔Effect of the invention〕

本発明によれば超音波振動子による内燃機関用燃料微粒
化装置の高電圧発生用コイルに流れる電流が最大になる
ように駆動回路の発振周波数を自動制御することにより
、振動子の燃料付着などによる負荷変動や温度特性およ
び発振回路の温度特性などにかかわりなく振動子の励振
周波数を常に安定して共振点付近に制御して最大出力か
えられるので装置効率を向上できる。
According to the present invention, by automatically controlling the oscillation frequency of the drive circuit so that the current flowing through the high voltage generating coil of a fuel atomization device for an internal combustion engine using an ultrasonic vibrator is maximized, fuel adhesion to the vibrator can be prevented. The device efficiency can be improved because the excitation frequency of the vibrator can always be stably controlled near the resonance point and the maximum output can be changed, regardless of load fluctuations, temperature characteristics, temperature characteristics of the oscillation circuit, etc.

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

第1図は本発明による内燃機関用燃料微粒化装置の駆動
回路の一実施例を示す全体端成図、第2図は第1図の超
音波振動子の出力特性図、第3図は第1図の発振回路の
回路側図、第4図は第1図の周波数制御回路の回路側図
、第5図は第1図の電流検出回路の回路側図である。 1・・・超音波振動子、2′・・・高電圧発生用コイル
、4゜5・・・パワートランジスタ、100・・・発振
回路、200・・・周波数制御回路、300・・・電流
検出回路。
FIG. 1 is an overall schematic diagram showing an embodiment of a drive circuit of a fuel atomization device for an internal combustion engine according to the present invention, FIG. 2 is an output characteristic diagram of the ultrasonic vibrator shown in FIG. 1, and FIG. 1, FIG. 4 is a circuit diagram of the frequency control circuit of FIG. 1, and FIG. 5 is a circuit diagram of the current detection circuit of FIG. 1. DESCRIPTION OF SYMBOLS 1... Ultrasonic transducer, 2'... Coil for high voltage generation, 4° 5... Power transistor, 100... Oscillation circuit, 200... Frequency control circuit, 300... Current detection circuit.

Claims (1)

【特許請求の範囲】[Claims] 1、内燃機関の燃料通路の途中に設けられた超音波振動
子と、該超音波振動子を励振する発振回路と、該発振回
路の出力を昇圧して上記超音波振動子に電圧を印加する
高電圧発生用コイルと、該高電圧発生用コイルの電流を
検出する電流検出回路と、上記発振回路の発振周波数を
上記超音波振動子の共振周波数よりはずれた所定周波数
から共振周波数に向けて変化させつつ上記高電圧発生用
コイルの電流が設定値に達した時点で上記電流検出回路
の出力により上記発振周波数の変化を停止させる周波数
制御回路とからなる内燃機関用燃料微粒化装置の駆動回
路。
1. An ultrasonic vibrator provided in the middle of a fuel passage of an internal combustion engine, an oscillation circuit that excites the ultrasonic vibrator, and boosting the output of the oscillation circuit to apply voltage to the ultrasonic vibrator. A high voltage generation coil, a current detection circuit that detects the current of the high voltage generation coil, and a current detection circuit that changes the oscillation frequency of the oscillation circuit from a predetermined frequency that is different from the resonance frequency of the ultrasonic transducer toward the resonance frequency. and a frequency control circuit that stops changing the oscillation frequency by the output of the current detection circuit when the current of the high voltage generating coil reaches a set value.
JP19888986A 1986-08-27 1986-08-27 Drive circuit of fuel atomizer for internal combustion engine Pending JPS6355358A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19888986A JPS6355358A (en) 1986-08-27 1986-08-27 Drive circuit of fuel atomizer for internal combustion engine

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19888986A JPS6355358A (en) 1986-08-27 1986-08-27 Drive circuit of fuel atomizer for internal combustion engine

Publications (1)

Publication Number Publication Date
JPS6355358A true JPS6355358A (en) 1988-03-09

Family

ID=16398622

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19888986A Pending JPS6355358A (en) 1986-08-27 1986-08-27 Drive circuit of fuel atomizer for internal combustion engine

Country Status (1)

Country Link
JP (1) JPS6355358A (en)

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