JPH0318136B2 - - Google Patents

Info

Publication number
JPH0318136B2
JPH0318136B2 JP10104682A JP10104682A JPH0318136B2 JP H0318136 B2 JPH0318136 B2 JP H0318136B2 JP 10104682 A JP10104682 A JP 10104682A JP 10104682 A JP10104682 A JP 10104682A JP H0318136 B2 JPH0318136 B2 JP H0318136B2
Authority
JP
Japan
Prior art keywords
bandwidth
piezoelectric element
resonance
resonant
frequency
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
JP10104682A
Other languages
Japanese (ja)
Other versions
JPS58216919A (en
Inventor
Makoto Yokoi
Akihito Inuzuka
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.)
Niterra Co Ltd
Original Assignee
NGK Spark Plug 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 NGK Spark Plug Co Ltd filed Critical NGK Spark Plug Co Ltd
Priority to JP10104682A priority Critical patent/JPS58216919A/en
Publication of JPS58216919A publication Critical patent/JPS58216919A/en
Publication of JPH0318136B2 publication Critical patent/JPH0318136B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L23/00Devices or apparatus for measuring or indicating or recording rapid changes, such as oscillations, in the pressure of steam, gas, or liquid; Indicators for determining work or energy of steam, internal-combustion, or other fluid-pressure engines from the condition of the working fluid
    • G01L23/22Devices or apparatus for measuring or indicating or recording rapid changes, such as oscillations, in the pressure of steam, gas, or liquid; Indicators for determining work or energy of steam, internal-combustion, or other fluid-pressure engines from the condition of the working fluid for detecting or indicating knocks in internal-combustion engines; Units comprising pressure-sensitive members combined with ignitors for firing internal-combustion engines
    • G01L23/221Devices or apparatus for measuring or indicating or recording rapid changes, such as oscillations, in the pressure of steam, gas, or liquid; Indicators for determining work or energy of steam, internal-combustion, or other fluid-pressure engines from the condition of the working fluid for detecting or indicating knocks in internal-combustion engines; Units comprising pressure-sensitive members combined with ignitors for firing internal-combustion engines for detecting or indicating knocks in internal combustion engines
    • G01L23/222Devices or apparatus for measuring or indicating or recording rapid changes, such as oscillations, in the pressure of steam, gas, or liquid; Indicators for determining work or energy of steam, internal-combustion, or other fluid-pressure engines from the condition of the working fluid for detecting or indicating knocks in internal-combustion engines; Units comprising pressure-sensitive members combined with ignitors for firing internal-combustion engines for detecting or indicating knocks in internal combustion engines using piezoelectric devices

Landscapes

  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Combustion & Propulsion (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

本発明は、内燃機関のシリンダ等に固結して、
該シリンダ内のノツキングの発生を検出するのに
用いる圧電共振型ノツクセンサにおいて、その共
振帯域幅調整方法に関する。 従来の圧電共振型ノツクセンサーは第1図の構
成になる。 図中、1は凹状のケースで、外底面中央に機関
のシリンダ壁に螺合する取付ボルト1aを突設し
ている。2は支持板で、前記ケースの内底面に載
置される。3は凹状の押え蓋で、閉端面がケース
の開口部を閉鎖し、開口縁が支持板の周辺に押圧
するようケース内に緊密に嵌挿される。このケー
ス1と支持板2と押え蓋3はケースの開口縁1b
を内側に折曲げ押え蓋の閉端面外周領域に係接す
ることによつて分離不能に固定される。4は金属
薄板41の片面にこれと同外径の円板状圧電素子
42を一体的に貼着してなる振動感知部材で、前
記金属薄板41の中央部下面から螺子軸5を突設
し、スペースナツト6を介装して該螺子軸5をケ
ース1の内底面に螺着することによつて、ケース
1内に支持される。 その他、前記押え蓋3には、端子9を植設し、
該端子9を導線10を介して圧電素子42の上面
電極42aと電気的に接続される。また下面電極
42bは螺子杵5によつてケース1と接続し、ボ
デイアースされる。 前記振動感知部材4は、その外径寸法によつて
ほぼ決定される共振周波数を、機関のノツク振動
周波数に略一致させることにより、ノツキングの
発生とともに、外周が上下に屈曲振動し、端子9
から最大出力が誘起される。 第2図の圧電素子の相対出力dBと、入力振動
波の周波数との関係を示すグラフにおいて、相対
出力dBは共振周波数f0のときに最大となり、そ
の前後で下降する。このことから、良好な出力を
得る上で、前記のように、共振周波数f0を、被検
出振動波(ノツキング振動波)の周波数と等しく
することが必要となる。一方、前記最大出力xよ
りも3dB度出力が低くなつても、出力信号として
は検出可能であつて、このため、この出力に対応
する周波数をf1、f2とすれば被検出振動波の周波
数がf1〜f2間の振動数であれば有効となる。 ここで、この周波数帯域f1〜f2の巾を共振帯域
巾B.Wという。 ところで、ノツク振動周波数は、種類、型式が
同一の機関であつても、機関構成部品のばらつき
や運転条件によつて変動し、このため共振帯域巾
B.Wが狭く、該巾からノツク振動周波数がずれ
ると、出力が低下して充分な検知が得られない。 また、共振帯域巾B.Wが広すぎても、機関に
はノツキング以外の種々の原因からなる振動波が
生ずるが、これらの振動波をも検出することとな
つて、正確な検知が得られない。従つて、共振帯
域巾B.Wは使用条件に適合した最適なものとす
る必要がある。 本発明は上述の要求に対応して共振帯域幅を最
適に調整する方法に係るものであり、圧電素子の
中心部に、円孔を外形と同心状に配し、その円孔
の内径を、共振帯域幅を増大させる場合には小さ
なものとし、共振帯域幅を減少させる場合には大
きなものとすることにより振動感知部材の共振帯
域幅を調整するようにしたものである。 すなわち、本発明者は、外径が等しく、かつ外
径と同心状に円孔aを形成してなる圧電素子4
2′を、前記円孔aの内径を異ならせて多数用意
し、第3図に示すように、各圧電素子42′を、
中心に透孔を設けた金属薄板41′の上面に接合
して振動感知部材4′を形成し、その透孔の上面
にはリング板7a及び電極板8を、下面にはリン
グ板7bを夫々当接して、該透孔にボルト(軸)
5′を通し、スペースナツト6を介してケース1
の内底面に螺合することにより前記振動感知部材
4′をケース1内に支持し、かつ圧電素子の上面
電極42′aを押え蓋3に植設した出力端子9a
に、下面電極42′bを同じくアース端子9bに
夫々接続してノツクセンサーを夫々構成し、各セ
ンサーにつき、共振帯域巾B.W、共振周波数f0
び出力電子VRについて計測した。その結果、第
5図のグラフで示されるように、共振周波数f0
ほとんど等しく、共振帯域巾B.Wのみが異なる
ことを知得した。 かかる実験の諸条件について記載する。 〈使用された部品の材質及び形状〉 ◎金属薄板の材質及び形状 材質;ニツケル合金 外径;15.6φ 内径;2φ 厚さ;0.2mm ◎圧電素子の材質及び形状 材質;チタン酸(TiO2) ジルコン酸(ZrO2) 鉛(pb)を焼結してなるPZTセラミツクス 外径;15.2φ 厚さ;0.25mm ◎リング板の形状 外径;3.4mm 内径;2mm 厚さ;1.00mm 〈実験方法〉 共振周波数f0は、リング板金属薄板の厚さ、形
状及び圧電素子の外径、厚さによつて変化するこ
とが知られている。そこで、これらのものを前記
数値の通り一定とし圧電素子の内径のみを異なら
せて第4図のセンサーを構成し、各センサーごと
に周波数測定器にかけて、オシログラフより共振
周波数f0(kHz)と、該共振周波数f0の相対出力
dBより3dB下がつた出力に対応する周波数の巾
(共振帯域巾B.W)と、出力電圧(VR)とを読み
とつた。 〈実験結果〉
The present invention can be fixed to a cylinder of an internal combustion engine, etc.
The present invention relates to a method for adjusting the resonance bandwidth of a piezoelectric resonance type knock sensor used to detect the occurrence of knocking in the cylinder. A conventional piezoelectric resonance type knock sensor has the configuration shown in FIG. In the figure, 1 is a concave case, and a mounting bolt 1a is provided protruding from the center of the outer bottom surface to be screwed into the cylinder wall of the engine. A support plate 2 is placed on the inner bottom surface of the case. Reference numeral 3 denotes a concave presser lid, which is tightly fitted into the case so that its closed end closes the opening of the case and the edge of the opening presses against the periphery of the support plate. This case 1, support plate 2, and presser cover 3 are the opening edge 1b of the case.
is fixed inseparably by bending it inward and engaging the outer peripheral area of the closed end surface of the presser cover. Reference numeral 4 denotes a vibration sensing member made by integrally adhering a disk-shaped piezoelectric element 42 having the same outer diameter to one side of a thin metal plate 41. A screw shaft 5 is provided protruding from the lower surface of the center of the thin metal plate 41. The screw shaft 5 is supported in the case 1 by screwing it into the inner bottom surface of the case 1 with a space nut 6 interposed therebetween. In addition, a terminal 9 is implanted in the presser cover 3,
The terminal 9 is electrically connected to the upper surface electrode 42a of the piezoelectric element 42 via a conducting wire 10. Further, the lower surface electrode 42b is connected to the case 1 by the screw punch 5 and is grounded to the body. The vibration sensing member 4 has a resonant frequency, which is approximately determined by its outer diameter, substantially equal to the knocking vibration frequency of the engine, so that when knocking occurs, the outer periphery of the vibration sensing member 4 bends vertically and vibrates, causing the terminal 9
Maximum power is induced from . In the graph of FIG. 2 showing the relationship between the relative output dB of the piezoelectric element and the frequency of the input vibration wave, the relative output dB reaches a maximum at the resonance frequency f 0 and decreases before and after that. Therefore, in order to obtain a good output, it is necessary to make the resonant frequency f 0 equal to the frequency of the detected vibration wave (knocking vibration wave) as described above. On the other hand, even if the output is 3 dB lower than the maximum output x, it can be detected as an output signal. Therefore, if the frequencies corresponding to this output are f 1 and f 2 , It is effective if the frequency is between f 1 and f 2 . Here, the width of this frequency band f 1 to f 2 is referred to as the resonance band width BW. Incidentally, even in engines of the same type and model, the knock vibration frequency varies depending on variations in engine components and operating conditions, and as a result, the resonance bandwidth
If the BW is narrow and the knock vibration frequency deviates from the width, the output will drop and sufficient detection will not be obtained. Furthermore, if the resonance bandwidth BW is too wide, vibration waves caused by various causes other than knocking are generated in the engine, and these vibration waves are also detected, making it impossible to obtain accurate detection. Therefore, the resonance bandwidth BW needs to be optimized to suit the usage conditions. The present invention relates to a method of optimally adjusting the resonance bandwidth in response to the above-mentioned requirements, in which a circular hole is arranged in the center of a piezoelectric element concentrically with the outer shape, and the inner diameter of the circular hole is The resonance bandwidth of the vibration sensing member is adjusted by making it smaller when increasing the resonance bandwidth and increasing it when decreasing the resonance bandwidth. That is, the present inventor has developed a piezoelectric element 4 having the same outer diameter and having a circular hole a formed concentrically with the outer diameter.
A large number of piezoelectric elements 42' are prepared with different inner diameters of the circular holes a, and as shown in FIG. 3, each piezoelectric element 42' is
The vibration sensing member 4' is bonded to the upper surface of a thin metal plate 41' having a through hole in the center, and a ring plate 7a and an electrode plate 8 are mounted on the upper surface of the through hole, and a ring plate 7b is mounted on the lower surface. Insert the bolt (shaft) into the through hole.
5' and case 1 via space nut 6.
The output terminal 9a supports the vibration sensing member 4' in the case 1 by screwing into the inner bottom surface of the output terminal 9a, and the upper surface electrode 42'a of the piezoelectric element is implanted in the holding lid 3.
Next, the lower electrodes 42'b were similarly connected to the ground terminal 9b to form knock sensors, and the resonance bandwidth BW, resonance frequency f0 , and output electron VR were measured for each sensor. As a result, as shown in the graph of FIG. 5, it was found that the resonant frequencies f 0 were almost the same, and only the resonant bandwidths BW were different. The conditions for such experiments will be described. <Material and shape of parts used> ◎Material and shape of thin metal plate Material: Nickel alloy Outer diameter: 15.6φ Inner diameter: 2φ Thickness: 0.2mm ◎Material and shape of piezoelectric element Material: Titanic acid (TiO 2 ) Zircon Acid (ZrO 2 ) PZT ceramics made by sintering lead (PB) Outer diameter: 15.2φ Thickness: 0.25mm ◎Ring plate shape Outer diameter: 3.4mm Inner diameter: 2mm Thickness: 1.00mm <Experimental method> Resonance It is known that the frequency f 0 changes depending on the thickness and shape of the thin metal ring plate and the outer diameter and thickness of the piezoelectric element. Therefore, we configured the sensor shown in Figure 4 by keeping these values constant as shown above and varying only the inner diameter of the piezoelectric element.We measured the resonance frequency f 0 (kHz) for each sensor by using a frequency measuring device, and measured it using an oscilloscope. , the relative output of the resonant frequency f 0
We read the frequency width (resonance band width BW) corresponding to the output that is 3 dB lower than dB and the output voltage (V R ). <Experimental result>

【表】 前記数値を第5図において、グラフで示す。 この結果によると、内径が小さくなるに従つ
て、共振周波数f0(kHz)はほとんど変化しない
が、共振帯域B.W(Hz)は、増大していくことが
示される。また出力電圧VRは漸減するが顕著で
はないことが示される。 このことから、内径を変えることによつて、共
振周波数f0をそのままにして共振帯域巾B.W(Hz)
を変えることができることが解る。この理由は定
かではないが、振動感知部材の振動は様々なベン
デイングモードによつて構成されるが、内径を小
さくすると、副次共振が顕在化して共振帯域巾
B.Wが増大するのではないかと、一応考察され
る。 本発明は、前記知見に基づき、圧電素子42′
に円孔aを形成することによつて、任意に共振帯
域巾B.Wを選定するものであり、ノツキング振
動波の周波数のばらつきが大きい場合には、内径
を小さくし、小さい場合には他の検出不要の振動
波が、被検出振動波とともに検出されるのを防止
するため内径を大きくして夫々形成することによ
り、極めて簡易に、最適な共振帯域巾B.Wを生
じることができ、しかもかかる共振帯域幅の調整
によつても、共振周波数f0はほとんど変化させな
いという優れた効果がある。 その他、本発明の共振帯域幅を適用した場合に
は、円孔aが形成されることにより、以下のよう
な付随的効果が生ずる。 すなわち金属薄板41′の中心部が露出するか
ら、第4図のように、ボルト5′の螺挿によつて
振動感知部材4′をケース1内に支持することが
でき、従来のように薄板41の下面に螺子杵5を
ロー付等によつて取付ける等の面倒な工作を要し
ず取付けが容易となる。 また、薄板41は圧電素子42′に比して可撓
性が高いから、円孔aから露出した中心部の薄板
aが良く撓んで、圧電素子42′の湾曲が良好と
なり、従来に比して高い出力を生ずる。このこと
は、円孔aの径が小さくなる程、出力電圧VR
低下することからも伺い知れる。 さらにまた、圧電素子42′と、金属薄板4
1′とは熱膨張係数が異なり、外気の温度変化に
より圧電素子42′と、薄板41の接合部で圧電
素子42′に亀裂を生ずることがあるが、前記円
孔aによつて接触面積が減少するから、前記損壊
が可及的に防止される。
[Table] The above numerical values are shown graphically in FIG. This result shows that as the inner diameter becomes smaller, the resonance frequency f 0 (kHz) hardly changes, but the resonance band BW (Hz) increases. It is also shown that the output voltage V R gradually decreases, but not significantly. From this, by changing the inner diameter, we can change the resonance band width BW (Hz) without changing the resonance frequency f 0 .
I understand that it is possible to change. The reason for this is not clear, but the vibration of the vibration sensing member is composed of various bending modes, but when the inner diameter is made smaller, secondary resonance becomes apparent and the resonance bandwidth becomes smaller.
It is considered that BW may increase. Based on the above findings, the present invention provides a piezoelectric element 42'
By forming a circular hole a in the hole a, the resonance bandwidth BW is arbitrarily selected.If the frequency variation of knocking vibration waves is large, the inner diameter is made small, and if it is small, other detection methods are used. In order to prevent unnecessary vibration waves from being detected together with the detected vibration waves, by forming each with a larger inner diameter, it is possible to extremely easily generate the optimum resonance bandwidth BW, and furthermore, such a resonance band Even by adjusting the width, there is an excellent effect that the resonant frequency f 0 hardly changes. In addition, when the resonance bandwidth of the present invention is applied, the following additional effects are produced by forming the circular hole a. That is, since the center of the thin metal plate 41' is exposed, the vibration sensing member 4' can be supported in the case 1 by screwing the bolt 5' as shown in FIG. The screw punch 5 can be easily attached without requiring troublesome work such as attaching the screw punch 5 to the lower surface of the screw 41 by brazing or the like. Further, since the thin plate 41 has higher flexibility than the piezoelectric element 42', the thin plate a at the center exposed from the circular hole a can be bent well, and the piezoelectric element 42' can be curved better than before. produces high output. This can be seen from the fact that the smaller the diameter of the circular hole a, the lower the output voltage V R becomes. Furthermore, a piezoelectric element 42' and a thin metal plate 4
1' has a different coefficient of thermal expansion, and cracks may occur in the piezoelectric element 42' at the junction between the piezoelectric element 42' and the thin plate 41 due to temperature changes in the outside air. Since the damage is reduced, the damage is prevented as much as possible.

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

第1図は、従来のノツクセンサーの縦断側面
図、第2図は、相対出力と入力振動波の周波数と
の関係を示すグラフ、第3図は、本発明を適用し
たノツクセンサーの縦断側面図、第4図は、圧電
素子の平面図、第5図は、本発明に係る実験結果
を示すグラフである。 4,4′;振動感知部材、41,41′;金属薄
板、42,42′;圧電素子、a;円孔。
Fig. 1 is a vertical side view of a conventional knock sensor, Fig. 2 is a graph showing the relationship between relative output and frequency of input vibration wave, and Fig. 3 is a longitudinal side view of a knock sensor to which the present invention is applied. , FIG. 4 is a plan view of the piezoelectric element, and FIG. 5 is a graph showing experimental results according to the present invention. 4, 4'; Vibration sensing member, 41, 41'; Metal thin plate, 42, 42'; Piezoelectric element, a; Circular hole.

Claims (1)

【特許請求の範囲】 1 金属薄板の一面に円板状圧電素子を一体に貼
着し、その共振周波数をノツク振動周波数に略一
致させてなる振動感知部材を、該薄板の中心から
下方に突出した軸によつて機関取付け用のケース
内に支持したものにおいて、 前記圧電素子の中心部に、円孔を外形と同心状
に配し、その円孔の内径を、共振帯域幅を増大さ
せる場合には小さなものとし、共振帯域幅を減少
させる場合には大きなものとすることにより振動
感知部材の共振帯域幅を最適に調整することを特
徴とする内燃機関用圧電共振型ノツクセンサーの
共振帯域幅調整方法。
[Scope of Claims] 1. A vibration sensing member made by integrally adhering a disc-shaped piezoelectric element to one surface of a thin metal plate and making its resonance frequency substantially match the knock vibration frequency is protruded downward from the center of the thin metal plate. A circular hole is arranged in the center of the piezoelectric element concentrically with the outer shape, and the inner diameter of the circular hole is set to increase the resonance bandwidth. The resonant bandwidth of a piezoelectric resonant sensor for an internal combustion engine is characterized in that the resonant bandwidth of a vibration sensing member is optimally adjusted by setting the resonant bandwidth to a small value when decreasing the resonant bandwidth, and increasing the resonant bandwidth when the resonant bandwidth is decreased. Adjustment method.
JP10104682A 1982-06-11 1982-06-11 Piezoelectric resonating type knock sensor for internal combustion engine Granted JPS58216919A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10104682A JPS58216919A (en) 1982-06-11 1982-06-11 Piezoelectric resonating type knock sensor for internal combustion engine

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10104682A JPS58216919A (en) 1982-06-11 1982-06-11 Piezoelectric resonating type knock sensor for internal combustion engine

Publications (2)

Publication Number Publication Date
JPS58216919A JPS58216919A (en) 1983-12-16
JPH0318136B2 true JPH0318136B2 (en) 1991-03-11

Family

ID=14290182

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10104682A Granted JPS58216919A (en) 1982-06-11 1982-06-11 Piezoelectric resonating type knock sensor for internal combustion engine

Country Status (1)

Country Link
JP (1) JPS58216919A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60256730A (en) * 1984-06-01 1985-12-18 Matsushita Electric Ind Co Ltd Space heating device
JPS6117916A (en) * 1984-07-04 1986-01-25 Matsushita Electric Ind Co Ltd Knock sensor

Also Published As

Publication number Publication date
JPS58216919A (en) 1983-12-16

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