JPS58111987A - Piezo-electric type alarm - Google Patents

Piezo-electric type alarm

Info

Publication number
JPS58111987A
JPS58111987A JP57210025A JP21002582A JPS58111987A JP S58111987 A JPS58111987 A JP S58111987A JP 57210025 A JP57210025 A JP 57210025A JP 21002582 A JP21002582 A JP 21002582A JP S58111987 A JPS58111987 A JP S58111987A
Authority
JP
Japan
Prior art keywords
frequency
piezoelectric vibrator
piezoelectric
self
resonance
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.)
Granted
Application number
JP57210025A
Other languages
Japanese (ja)
Other versions
JPH0139595B2 (en
Inventor
工藤 道夫
龍夫 深海
林部 林平
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to JP57210025A priority Critical patent/JPS58111987A/en
Publication of JPS58111987A publication Critical patent/JPS58111987A/en
Publication of JPH0139595B2 publication Critical patent/JPH0139595B2/ja
Granted legal-status Critical Current

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  • Piezo-Electric Transducers For Audible Bands (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 この発明は、圧電型振動子を用いた圧電式警報器に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a piezoelectric alarm using a piezoelectric vibrator.

従来、圧電型振動子を用いた圧電式警報器では、鳴動周
波数は圧電型振動子の屈曲振動による共振周波数で決定
され、その周波数は2〜3KH2程度の極めて高い単振
動音となり、ブザー等の警報器の音色としてはあまり適
当ではなかった。
Conventionally, in a piezoelectric alarm device using a piezoelectric vibrator, the ringing frequency is determined by the resonance frequency caused by the bending vibration of the piezoelectric vibrator, and the frequency is an extremely high simple harmonic sound of about 2 to 3 KH2, which is similar to that of a buzzer, etc. The tone was not very appropriate for an alarm.

本発明は上記問題点を解決するためになされたもので、
圧電型振動子の周波数特性を多峰特性にするとともに、
変調回路を接続して搬送周波数と側帯波周波数とをそれ
ぞれ圧電型振動子の共振点に一致させることにより、音
色に幅があり、lKH2以下の可聴音を発する圧電式警
報器を提供することを目的とするものである。
The present invention has been made to solve the above problems,
In addition to making the frequency characteristics of the piezoelectric vibrator multimodal,
It is an object of the present invention to provide a piezoelectric alarm device that has a wide range of tones and emits an audible sound of 1KH2 or less by connecting a modulation circuit and matching the carrier frequency and sideband frequency to the resonance points of a piezoelectric vibrator. This is the purpose.

以下、本発明の実施例を図面に基づいて詳細に説明する
。
Embodiments of the present invention will be described in detail below with reference to the drawings.

第1図は圧電型振動子の平面図を示すもので、圧電素子
1は、長辺a、短辺すの方形の金属板2に接着剤で接合
され、これらは更に、平面部分が金属板2と相似形であ
って、周辺部はしばり加工されているダイヤフラム3と
接着されて全体として圧電型振動子4を構成している。
FIG. 1 shows a plan view of a piezoelectric vibrator, in which a piezoelectric element 1 is bonded with an adhesive to a rectangular metal plate 2 with a long side a and a short side a. The piezoelectric vibrator 4 has a similar shape to the piezoelectric vibrator 2, and is bonded to a diaphragm 3 whose peripheral portion is bound to form a piezoelectric vibrator 4 as a whole.

このような構造の圧電型振動子では、長辺方向及び短辺
方向の屈曲振動が共存することになり、振動周波数は金
属板2の各寸法a、bに関係する。例えば、長辺a+a
a40mm。
In a piezoelectric vibrator having such a structure, bending vibrations in the long side direction and the short side direction coexist, and the vibration frequency is related to the dimensions a and b of the metal plate 2. For example, long side a+a
a40mm.

短辺bw3Q+uaの場合、第2図に示すように、発生
音量と周波数fとの関係を示す周波数特性は2つの共振
点をもつ双峰特性となり、両共振周波数XI。
In the case of the short side bw3Q+ua, as shown in FIG. 2, the frequency characteristic showing the relationship between the generated sound volume and the frequency f is a bimodal characteristic with two resonance points, and both resonance frequencies XI.

X2の間隔Δfは約400H2であった。The interval Δf of X2 was approximately 400H2.

第3図は、第1図に示す圧電型振動子4を振幅変調波で
励振する回路を示すもので、トランジスタTrlと抵抗
R4、R5、R6とにより前置増幅器を構成している。
FIG. 3 shows a circuit for exciting the piezoelectric vibrator 4 shown in FIG. 1 with an amplitude modulated wave, and a preamplifier is configured by a transistor Trl and resistors R4, R5, and R6.

この前置増幅器の出力側には、抵抗R1を介してダーリ
ントン接続したトランジスタTr2゜Tr3よりなる一
電力増幅器を接続している。電力増幅器の出力側(トラ
ンジスタTr3のエミッタ)には、保護抵抗R4,バイ
パス容量CIを介して昇圧トランスTの一次側が接続さ
れている。昇圧トランスTの二次側には圧電型振動子4
と互いに並列接続されている抵抗R3,位、相補慣用容
量C2を直列に□0..−い64□1ム、□工4よ1、
□動子4に流れる電流に比例するから、この分割電圧を
結合容量C3を介してトランジスタTrlのベースに正
帰還させて自励発振回路を構成している。
A power amplifier consisting of Darlington-connected transistors Tr2 and Tr3 is connected to the output side of this preamplifier through a resistor R1. The output side of the power amplifier (the emitter of the transistor Tr3) is connected to the primary side of the step-up transformer T via a protection resistor R4 and a bypass capacitor CI. A piezoelectric vibrator 4 is installed on the secondary side of the step-up transformer T.
and the resistor R3, which are connected in parallel with each other, and the complementary common capacitor C2 are connected in series with □0. .. -64□1mu, □engineering 4yo1,
□Since it is proportional to the current flowing through the actuator 4, this divided voltage is positively fed back to the base of the transistor Trl via the coupling capacitor C3 to form a self-excited oscillation circuit.

又、トランジスタTriのコレクタとトランジスタTr
2のベースとの間には抵抗R1,R2、ダイオードDI
、D2よりなる変調回路を接続している。5は局部発振
器である。
In addition, the collector of the transistor Tri and the transistor Tr
2, resistors R1 and R2, and a diode DI are connected to the base of
, D2 is connected to the modulation circuit. 5 is a local oscillator.

次に、回路動作について、第3図〜第5図を参“照して
説明する。
Next, the circuit operation will be explained with reference to FIGS. 3 to 5.

自励発振回路は昇圧トランスTの二次胱起電圧を圧電振
動子4に印加し、これに流れる電流に比例した電圧を抵
抗R3より取り出して結合容量C3を介して、トランジ
スタTriのベースに正帰還している。従って、この自
励発振回路では第2図に示す共振点を示す周波数XIあ
るいはx2に相当する周波数で自励発振する。従って、
トランジスタTrlのコレクタには、第4図(a)に示
すような電圧波形の自励発振信号が出力しており、この
信号が搬送波信号となる。一方、局部発振器5からは第
4図(b)に示す変調波信1号が出力する。ここで、局
部発振器5の変調波信号(第4図(b))はダイオード
D2.D1.  抵抗R1,R2よりなる変調回路に印
加される。
The self-excited oscillation circuit applies the secondary electromotive force of the step-up transformer T to the piezoelectric vibrator 4, extracts a voltage proportional to the current flowing through the piezoelectric vibrator 4 from the resistor R3, and applies a positive voltage to the base of the transistor Tri via the coupling capacitor C3. He is returning. Therefore, this self-excited oscillation circuit performs self-excited oscillation at a frequency corresponding to the frequency XI or x2 indicating the resonance point shown in FIG. Therefore,
A self-oscillating signal having a voltage waveform as shown in FIG. 4(a) is outputted to the collector of the transistor Trl, and this signal becomes a carrier wave signal. On the other hand, the local oscillator 5 outputs a modulated wave signal 1 shown in FIG. 4(b). Here, the modulated wave signal of the local oscillator 5 (FIG. 4(b)) is transmitted through the diode D2. D1. It is applied to a modulation circuit consisting of resistors R1 and R2.

この時、0−tlの期間、即ち、第4図(b)に示す出
力電圧がOvの期間では、ダイオードD2はオフ、ダイ
オードD1はトランジスタTrlのコレクタ電圧(第4
図(a))がOvの時オフ、+VVの時オンとなるから
、トランジスタTr2のベースには、第4図(C)に示
すように、トランジスタTrlのコレクタ電圧が抵抗R
1,R2によって分圧され減衰されて出力する。
At this time, during the period 0-tl, that is, the period when the output voltage is Ov shown in FIG.
Figure 4(a)) is off when it is Ov and turned on when it is +VV, so the collector voltage of the transistor Trl is connected to the base of the transistor Tr2 by the resistor R, as shown in Figure 4(C).
1 and R2, the voltage is divided and attenuated and output.

次いで、tl〜t2の期間、即ち、第4図(b)に示す
出力電圧が+vVの期間では、ダイオードD2はオン、
ダイオードD1はオフとなるから、トランジスタTr2
のベース(B点)には、第4図(C)に示すように、A
点の電圧がそのまま現われる。以上のようにして、第4
図(C)に示すB点の電圧はトランジスタTr2.Tr
3により電力増幅された後、昇圧トランスTによって昇
圧、直流分除去されて、二次側の0点には第4図(d)
に示す振幅変調波が出力し、圧電型振動子4に印加され
、これを駆動する。ここで、振幅変調された変調出力の
周波数スペクトルのうち、基本スペクトルは第5図に示
すように、自励発振周波数(搬送波周波数) fo、変
調波周波数fiとすれば、側帯波周波数は10オfiと
なる。従って(自動発振周波数fOは第2図に示す共振
周波数XI (あるいはX2)に一致しており、側帯波
周波数fo±f1のいずれか一方が共振周波数x2(あ
るいはXI)に一致する。即ち、変調周波数fiは第2
図に示す周波数間隔4fに等しく選べばよい。
Next, during the period from tl to t2, that is, during the period when the output voltage is +vV shown in FIG. 4(b), the diode D2 is turned on.
Since the diode D1 is turned off, the transistor Tr2
As shown in Figure 4 (C), at the base (point B) of
The voltage at the point appears as is. As described above, the fourth
The voltage at point B shown in the diagram (C) is the voltage at the transistor Tr2. Tr
After the power is amplified by step-up transformer T, the voltage is boosted by step-up transformer T, and the DC component is removed.
An amplitude modulated wave shown in is outputted and applied to the piezoelectric vibrator 4 to drive it. Here, among the frequency spectrum of the amplitude-modulated modulated output, the fundamental spectrum is the self-oscillation frequency (carrier frequency) fo and the modulated wave frequency fi, as shown in Fig. 5, the sideband frequency is 10 ohms. It becomes fi. Therefore, (the automatic oscillation frequency fO matches the resonant frequency XI (or X2) shown in Fig. 2, and one of the sideband frequencies fo±f1 matches the resonant frequency x2 (or XI). The frequency fi is the second
It may be selected to be equal to the frequency interval 4f shown in the figure.

なお、上述の実施例では、発振器を局部発振器として説
明したがこれに限らず他の発振器でもよく、又さらに進
んで圧電型振動子4の自動発振信号を分周してなる自励
発振器でもよい。
In the above embodiments, the oscillator was described as a local oscillator, but the oscillator is not limited to this, and may be any other oscillator, or may go further and may be a self-excited oscillator formed by frequency-dividing the automatic oscillation signal of the piezoelectric vibrator 4. .

以上述べたように、本発明によれば圧電型振動子の周波
数特性を多峰特性にするとともに、変調回路を接続して
変調出力を印加して、搬送波周波数と側帯波周波数とを
それぞれ圧電型振動子の共振点の周波数に一致させたの
で、音色に幅があり、I KH2以下の可聴音を発生さ
せることができ、聴感上優れた警報器を得ることができ
る。
As described above, according to the present invention, the frequency characteristics of the piezoelectric vibrator are made multimodal, and a modulation circuit is connected to apply a modulated output, so that the carrier frequency and the sideband frequency are respectively changed to the piezoelectric vibrator. Since the frequency is made to match the resonance point of the vibrator, it is possible to generate an audible sound with a wide range of tones and below IKH2, and thus an alarm device with excellent audibility can be obtained.

以上本発明につき、好適な実施例を挙げて種々説明した
が、本発明はこの実施例に限定されるものではなく、発
明の精神を逸脱しない範囲内で多くの改変を施し得るの
はもちろんのことである。
The present invention has been variously explained above with reference to preferred embodiments, but the present invention is not limited to these embodiments, and it goes without saying that many modifications can be made without departing from the spirit of the invention. That's true.

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

図面は本発明の実施例を示すもので、第1図は圧電型振
動子の平面図、第2図は第1図に示す圧電型振動子の発
生音量と周波数との関係を示す周波数特性図、第3図は
回路図、第4図は各部の波形図、第5図は周波数スペク
トル図である。 l・・・・圧電素子、 2・・・・金属板、 3・・・
・ダイヤフラム、 4・・・・圧電型振動子、 5・・
・・局部発振器、 a・・・・長辺、 b・・・・短辺
、  XI。 X2・・・・共振周波数+  Tri、Tr2+Tr3
・・・・トランジスタ、  R1,R2,R3,R4,
R5,R6;;−・・抵抗、  CI、C2,C3・・
・・容量、 T・・・・トランス、  DI、D2・・
・・ダイオード。 特許出願人 工藤道夫(他2名) −わ11λ1 弔2図 う′ト 第3図 一澗 第1図 ・ぷ5図
The drawings show an embodiment of the present invention, and FIG. 1 is a plan view of a piezoelectric vibrator, and FIG. 2 is a frequency characteristic diagram showing the relationship between the generated sound volume and frequency of the piezoelectric vibrator shown in FIG. 1. , FIG. 3 is a circuit diagram, FIG. 4 is a waveform diagram of each part, and FIG. 5 is a frequency spectrum diagram. l...piezoelectric element, 2...metal plate, 3...
・Diaphragm, 4...Piezoelectric vibrator, 5...
...local oscillator, a...long side, b...short side, XI. X2...Resonance frequency + Tri, Tr2+Tr3
...transistor, R1, R2, R3, R4,
R5, R6; -...Resistance, CI, C2, C3...
...Capacity, T...Transformer, DI, D2...
··diode. Patent application Artificial Fuji Michio (and 2 others) -W11λ1 Funeral 2 Figure U'to Figure 3 Ichiran Figure 1 and P5

Claims (1)

【特許請求の範囲】 1、圧電素子と金属板とを接合してあり、周波数特性が
複数の共振点を持つ多峰特性を示す圧電型振動子と、 この圧電型振動子の屈曲振動により自励発振する自励発
振回路の自励発振信号を搬送波とするとともに、発振器
からの変調波により上記搬送波を変調する回路と を具備し、上記圧電型振動子に変調出力を印加して、上
記共振点の1つに上記搬送波の周波数を、他の共振点に
側帯波周波数をそれぞれ一致させたことを特徴とする圧
電式警報器。
[Claims] 1. A piezoelectric vibrator in which a piezoelectric element and a metal plate are bonded together and whose frequency characteristics exhibit multimodal characteristics with multiple resonance points; The circuit includes a circuit that uses a self-excited oscillation signal of a self-excited oscillation circuit that performs excitation oscillation as a carrier wave, and modulates the carrier wave with a modulated wave from an oscillator, and applies a modulated output to the piezoelectric vibrator to generate the resonance. A piezoelectric alarm device characterized in that the frequency of the carrier wave is made to match one of the points, and the sideband frequency is made to match the frequency of the other resonance point.
JP57210025A 1982-11-29 1982-11-29 Piezo-electric type alarm Granted JPS58111987A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57210025A JPS58111987A (en) 1982-11-29 1982-11-29 Piezo-electric type alarm

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57210025A JPS58111987A (en) 1982-11-29 1982-11-29 Piezo-electric type alarm

Publications (2)

Publication Number Publication Date
JPS58111987A true JPS58111987A (en) 1983-07-04
JPH0139595B2 JPH0139595B2 (en) 1989-08-22

Family

ID=16582566

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57210025A Granted JPS58111987A (en) 1982-11-29 1982-11-29 Piezo-electric type alarm

Country Status (1)

Country Link
JP (1) JPS58111987A (en)

Also Published As

Publication number Publication date
JPH0139595B2 (en) 1989-08-22

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