JPS5892908A - Detector using piezo vibrator - Google Patents

Detector using piezo vibrator

Info

Publication number
JPS5892908A
JPS5892908A JP19211981A JP19211981A JPS5892908A JP S5892908 A JPS5892908 A JP S5892908A JP 19211981 A JP19211981 A JP 19211981A JP 19211981 A JP19211981 A JP 19211981A JP S5892908 A JPS5892908 A JP S5892908A
Authority
JP
Japan
Prior art keywords
electrodes
vibrator
resistance
piezoelectric vibrator
detection
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
JP19211981A
Other languages
Japanese (ja)
Other versions
JPH0245802B2 (en
Inventor
Tetsuo Konno
哲郎 今野
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.)
Seikosha KK
Original Assignee
Seikosha KK
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 Seikosha KK filed Critical Seikosha KK
Priority to JP19211981A priority Critical patent/JPS5892908A/en
Publication of JPS5892908A publication Critical patent/JPS5892908A/en
Publication of JPH0245802B2 publication Critical patent/JPH0245802B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01DMEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D5/00Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
    • G01D5/12Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means
    • G01D5/14Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Testing Or Calibration Of Command Recording Devices (AREA)
  • Transmission And Conversion Of Sensor Element Output (AREA)
  • Investigating Or Analyzing Materials By The Use Of Fluid Adsorption Or Reactions (AREA)

Abstract

PURPOSE:To provide direct digital processing by a compact simple construction wherein two vibrating regions are formed on a piezo vibrator and, as a back electrode, a material whose electric resistance changes in response to an object to be detected is used to detect the object based on the difference in oscillating frequency between the vibrating regions. CONSTITUTION:There is shown a crystal vibrator P as a piezo vibrator and one of the surfaces is provided with two pairs of single side driving electrodes E11, E12 and E21, E22, the electrodes forming vibrating regions A1, A2, respectively. The other surface of the crystal vibrator P is used as a free surface, whereas back electrodes B1, B2 are formed on the back surfaces of the electrodes E11, E12 and E21, E22. Then an oscillation circuit OS1 is formed by connecting a C-MMOS invertor V1, a resistor R1 and capacitors C11, C12 to the electrodes E11, E12, whereas an oscillation circuit OS2 is formed by connecting a C-MOS invertor V2, a resistor V2 and capacitors C21, C22 to the electrodes E21, E22. There is also shown a mixer M in the Figure.

Description

【発明の詳細な説明】 本免明扛圧電畿動子を用いた検出装置に蘭するものでる
る〇 例えば、光、磁気、總度、湿度、ガス尋を検出するセン
ナが捕々開発されているが、これらの検出出力t−vイ
クロコンピュータ尋でデジタル処理する場合には、イン
ターフェイスとして五−り変換器を必要とすることが多
く、−成約に複雑になるものでめった。
[Detailed Description of the Invention] This invention relates to detection devices using piezoelectric actuators. For example, sensors that detect light, magnetism, temperature, humidity, and gas temperature have been rapidly developed. However, when these detection outputs are digitally processed using a TV microcomputer, a five-way converter is often required as an interface, which is rarely complicated.

そこで本発明は直接デジタル処理が可能でたつ島い検出
NIK’を有したコンパクトな圧電振動子を用いた検出
装置を提供するものである。
Therefore, the present invention provides a detection device using a compact piezoelectric vibrator having a small detection NIK' which can be directly digitally processed.

以下本発明の一実施@II−−面に基づいて説明する。EMBODIMENT OF THE INVENTION Hereinafter, one implementation of the present invention will be explained based on aspect II.

第1図において、Pは圧電振動子である水晶撫勤子でそ
の一面には2対の片面駆動用亀4Nmm112 > l
びWel、1ast形成し、それぞれ畿勤績域ム鴬、ム
sk−形成している0また水晶伽勤子Pの他FiJは自
田面となっており、電極111*ll−およびlll5
コ■の背面ににそrt(J31ir’面電1!Bs 、
Ih  ’r影形成てめる0 そり、?電極Ill m IIs K BtlA 2図
のzうにO−hiMO8インバータv1.抵抗R1j?
よび負荷容量’1ieOts k妥続して発fi回路0
81を構成し、電極E11゜1■にqC−MO8イレバ
ータvs、抵抗R3−よび負荷容t 0shOsnk接
続して発振1路Oam k構成している。Mはミキサで
るる。
In Fig. 1, P is a crystal vibrator which is a piezoelectric vibrator, and on one side there are two pairs of single-sided driving tortoises 4Nmm112>l.
and Wel and 1ast are formed, and the electrodes 111*ll- and lll5 are formed, respectively.
On the back of the
Ih 'r shadow formation 0 sled? Electrode Ill m IIs K BtlA 2 O-hiMO8 inverter v1. Resistance R1j?
and load capacitance '1ieOtsk continues to generate fi circuit 0
A qC-MO8 elevator, a resistor R3, and a load capacitor t0shOsnk are connected to the electrode E11゜1■ to form a single oscillation path Oamk. M is for mixer.

以上の#既において、水晶畿−子Pの一面は自由画とな
っているため1tRjII+領域ム1eAlの等価回路
は第5−のごとく表わされる。すなわち、両面動形の等
ll1lI−路Km抗分ダ8と容量分O8とが直列費続
石れたものとなって′いる。この抵抗分R8は自由面上
に形成された背面電極BゆるいはB、の電気抵抗に1っ
て形成されるtので、仁の抵抗値によって各振IIJ1
iI域の抛撫周波aは第4−のごとく変化する〇 そこで背面亀@B>あるいはB1のいずれか一方に特定
の検出河朧に感応してIE電気抵抗変化するセンサ用材
料2用いるとともに他方に上記検出対象に感Aもシない
ものt用いることに1!l1%q!rMjR勤領域の発
掘周波数の差η為ら対象を検出できる。
In the above #, since one surface of the crystal glass P is a free image, the equivalent circuit of 1tRjII+area 1eAl is expressed as 5th-. That is, the double-sided moving type equal 1111I-path Km resistor 8 and the capacitor 08 are connected in series. This resistance R8 is formed by 1 to the electrical resistance of the back electrode B formed on the free surface, so it depends on the resistance value of the back electrode B, so each swing IIJ1
The stroke frequency a in the iI region changes as shown in No. 4- Therefore, the sensor material 2 that changes the IE electrical resistance in response to a specific detection blur is used for either the back turtle @B> or B1, and the other 1 to use something that does not have any sensitivity to the above detection target! l1%q! The target can be detected from the difference η in the excavation frequencies of the rMjR working region.

1ず光センサとして使用する場合について述べるO牛導
体の内部光電効果を利用した光センナの9ち光導電効果
形の%Dは光量によってa抗が変化する。したかって、
例えば背面111k B*の材料としてca日、06B
m、PbEl、pbs=、工nAs、工n  sb。
First, we will discuss the case of using it as an optical sensor.The %D of the photoconductive effect type optical sensor that utilizes the internal photoelectric effect of the conductor changes its a resistance depending on the amount of light. I wanted to,
For example, the material for the back 111k B* is ca day, 06B
m, PbEl, pbs=, nkAs, nk sb.

Hg1−x Odz Te  (X電α2)elF”用
いれば、光量によって抵抗分1’18か第5図のごとく
変化する。すなわち、元麓によって第2図の発掘回路0
町の発掘周波数が変化する〇 一方背面電極B、として、光による影II!ir受けな
いムU等髪用いることによって、発条回路OS1゜08
雪の発伽周tlL数の差から光量を検出するCとができ
る。すなわち第2図のミキサM′からの出力周波数r計
数することによって光量を検出できる。
Hg1-x Odz Te (X-electron α2)elF", the resistance changes depending on the amount of light as shown in Figure 5. In other words, the excavation circuit 0 in Figure 2 depends on the
The excavation frequency of the town changes 〇 On the other hand, as the back electrode B, the shadow caused by the light II! By using hair that does not receive IR, the firing circuit OS1゜08
It is possible to detect the amount of light from the difference in the number of snow peaks tlL. That is, the amount of light can be detected by counting the output frequency r from mixer M' in FIG.

つぎに磁気センtとして使用する場合には、電子移動度
の大きい工n  sb等の■−■族化合物半導体を利用
した磁気抵抗素子を背向電極B1に用いればよLnoc
nは第6図示のような磁気−抵抗特性を示す。−万背面
亀1kBmには、磁気による影響を愛社ないAU等11
−#4Vhればよい。
Next, when using it as a magnetic center, a magnetoresistive element using a ■-■ group compound semiconductor such as Lnoc with high electron mobility may be used for the back electrode B1.
n indicates magneto-resistance characteristics as shown in FIG. - For 1kBm, there are 11 AUs etc. that are not affected by magnetism.
-#4Vh is sufficient.

また温MILセンサとして使用する場合には、温度にL
って抵抗が変化するナーミスタ、ポジスタ用材料r*t
hlt他B1として用い、背向電極B、  として框ム
U等を用いればよい。
Also, when used as a temperature MIL sensor, L
Materials for nermistors and posisters whose resistance changes
hlt etc. may be used as the electrode B1, and the frame U may be used as the back electrode B and the frame U.

さらに1ガスセンサとして用いる場合には、背面亀憶B
1としてn形半導体あるい框P形牛導体を用いれば工い
。内えば、n形半導体のガス磯度−抵抗特性は環元形ガ
スのa層によって第7嫡の曲−ものごとくなり、酸化形
方スの吸着に1って第7−の曲−1雪のごとくなる0ま
たP形半導体の場合に、上記と框逆=に還元形ガスの吸
着によって抵抗が増大し、順化形ガスの吸着に1って抵
抗か減少する0この場合にも背面亀禽B、としてはAU
等を用%AjLば工い。
In addition, when used as a single gas sensor, the rear camera memory B
This can be done by using an n-type semiconductor or a p-type conductor as 1. In other words, the gas resistance characteristics of an n-type semiconductor become like the 7th curve due to the a-layer of the cyclic gas, and the adsorption of oxidized squares becomes 1 and the 7th curve becomes 1 snow. 0 Also, in the case of a P-type semiconductor, the resistance increases due to the adsorption of the reduced gas, and the resistance decreases by 1 due to the adsorption of the acclimatized gas. Bird B, as for AU
If you use %AjL etc.

また、湿度センサとして使用する場合には、finol
  等の湿度によって抵抗か変化するtのt用いる。
Also, when used as a humidity sensor, finol
The resistance of t changes depending on the humidity.

8n01  の湿度−抵抗籍性を示した9が第8図でる
る。この場合には、背面電極B11/c債水性のコーテ
ィングkJiiして2くCとにLジムuK限らnずどの
よ5を物質でもよい0 な2この場合に水j!IfEIIJ子としてYカット畿
動子を用いると、その共振局yLIILか温度に対して
直融的に変化するため発畿(ロ)路OB雪の発伽周友数
〃為ら温[k検出する仁とができ、同時にミキサMの出
力周数数〃為ら湿R’を検出することかできる。
9 showing the humidity-resistance characteristics of 8n01 is shown in FIG. In this case, the back electrode B11/c has a water-based coating kJii and 2C and L Jim uK, but any substance may be used.0 In this case, water j! If a Y-cut transducer is used as the IfEIIJ element, its resonance station yLIIL changes directly with temperature, so the temperature [k is detected] At the same time, the humidity R' can be detected from the output frequency of the mixer M.

以上のように本発明によれば、一つの圧電撫動子上に2
@所の伽wjJ漬域を形成し一方の伽動−城の背向電極
と・して検出対象に感応して電気抵抗が変化する物質を
用^各条動領域の抛畿周tIN、、数の差ρ為ら対象を
検出するようkしたので、極めて小型で簡単な構成の検
出装[111−提供できし!>” 4ム−D変換器を介
することな(lljlデジタル処理か行なえる0 また検出対象による電気抵抗の変化は極ぬて顕著なもの
でるるため1IIIl槓度の検出が行なえる。
As described above, according to the present invention, there are two
@A substance whose electrical resistance changes in response to the object to be detected is used as the back electrode of one of the oscillation regions to form the oscillation region of the oscillation region. Since the object was detected based on the difference in number ρ, a detection device with an extremely small and simple configuration [111- could be provided!] >'' Digital processing can be performed without going through a 4μ-D converter. Also, since the change in electrical resistance due to the object to be detected is extremely significant, it is possible to detect 1IIIl degrees of force.

さらに、同−圧電振一子上に、二つの畿勘慎域か形成さ
nているため、各々の条部領域の周波数温度時性は同じ
ものとなる0そのため、発掘周波数の差には、温fIL
変動による誤差成分に入らないことになる0
Furthermore, since two ridge-cut regions are formed on the same piezoelectric vibrator, the frequency-temperature-temporality of each striation region is the same.Therefore, the difference in excavation frequency is Hot fIL
0, which will not be included in the error component due to fluctuations

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

第1図は不発明の一実施例における圧電伽動子の止面ン
Lび背面図、第2−に第1図の圧電懺勤子を用いた不発
明の一実施例の電気1g1wI図、第3図は片面本鯛形
水晶m1IJ子の等価回路図、第4図に背面1憔の抵抗
分と妬伽周波数との関係を示した時性図、第5融扛光量
と光導亀効来形材料の抵抗との@gIA1!−示した骨
性図、第6図は磁気抵抗軍子の磁界−抵抗骨性を示した
特性図、第7図an形半導体のガス濃度−抵抗骨性を示
した骨性図、第8図は81103のg1度−抵抗特性r
示した特性図であるO P・・・・・・圧電振動子 ”11 m ”11 m m11 m m11 ”””
片面駆動用電他ムle’l・・・・・・畿動領域 BlmBM ・・・・・・背面電極 O8,,08m・・・・・・発条回路 輩・・・・・・ミキサ 第1図 第2図 S2 第3図 第4図 →R5 第5図 第7因 xi’r    が゛スジ1艷→ 第6図 第8図 湘対湿度→
FIG. 1 is a top view and rear view of a piezoelectric transducer according to an embodiment of the invention, and FIG. 2 is an electrical diagram of an embodiment of the invention using the piezoelectric transducer of FIG. 1. Fig. 3 is an equivalent circuit diagram of a single-sided true sea bream-shaped crystal m1 IJ, Fig. 4 is a time diagram showing the relationship between the resistance of the back surface and the frequency, and the fifth fusion light amount and light guide effect. @gIA1 with resistance of shaped material! -Boneity diagram shown in Figure 6 is a characteristic diagram showing magnetic field-resistance bone property of magnetoresistive element, Figure 7 is a bone diagram showing gas concentration-resistance bone property of an-type semiconductor, Figure 8 is the g1 degree-resistance characteristic r of 81103
The characteristic diagram shown is O P...Piezoelectric vibrator "11 m"11 m m11 m m11 """
Single-sided driving electric current......Witling area BlmBM...Back electrode O8,,08m......Spring circuit...Mixer Figure 1 Fig. 2 S2 Fig. 3 Fig. 4 → R5 Fig. 5 Fig. 7 factor

Claims (1)

【特許請求の範囲】 2対の片面駆動用IIL億を圧電振動子の一方の向上に
形成して上記圧電振動子上に2i1所の畿勤偵域τ形成
し、 一方の対の片面駆−用電極の背面に検出対象に感応して
電気抵抗が変化する* ’j[k用いて背面電極を形成
し、 他の灼の片面属鯛用電禽の背面に、上記検出対象に感応
しない背面電極髪形成し、 上記各撫動績域を用いて2つの殆珈口路を構成し、 この各発振1gl路の出力周波数の差を検出する検出商
略に&けた ことt待機とする圧電振動子を用いた検出fe llk
 。
[Scope of Claims] Two pairs of single-sided drive IILs are formed on one side of the piezoelectric vibrator to form a 21-point horizontal rectangle τ on the piezoelectric vibrator, and one pair of single-sided drive IILs is formed on one side of the piezoelectric vibrator. The electrical resistance changes in response to the detection target on the back side of the electrode. The electrode hair is formed, and the above-mentioned stroking areas are used to form two almost radial channels, and the detection strategy is to detect the difference in the output frequency of each oscillating 1gl channel, and the piezoelectric vibration is used to wait for an order of magnitude. Detection using child fe llk
.
JP19211981A 1981-11-30 1981-11-30 Detector using piezo vibrator Granted JPS5892908A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19211981A JPS5892908A (en) 1981-11-30 1981-11-30 Detector using piezo vibrator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19211981A JPS5892908A (en) 1981-11-30 1981-11-30 Detector using piezo vibrator

Publications (2)

Publication Number Publication Date
JPS5892908A true JPS5892908A (en) 1983-06-02
JPH0245802B2 JPH0245802B2 (en) 1990-10-11

Family

ID=16285980

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19211981A Granted JPS5892908A (en) 1981-11-30 1981-11-30 Detector using piezo vibrator

Country Status (1)

Country Link
JP (1) JPS5892908A (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59217145A (en) * 1983-05-26 1984-12-07 Fujihira Kogyo Kk Total sugar amount measuring apparatus
JPH01282418A (en) * 1988-05-09 1989-11-14 Hitachi Ltd Piezo-electric type physical quantity detector
JPH0357932A (en) * 1989-07-27 1991-03-13 Agency Of Ind Science & Technol Crystal temperatuer sensor for cryogenic temperature
JP2000283905A (en) * 1999-03-30 2000-10-13 Noboru Koyama Multichannel qcm sensor device
JP2010503116A (en) * 2006-09-06 2010-01-28 スリーエム イノベイティブ プロパティズ カンパニー Spatially distributed remote sensors
JP2012008029A (en) * 2010-06-25 2012-01-12 Nippon Dempa Kogyo Co Ltd Sensing device
US9086338B2 (en) 2010-06-25 2015-07-21 Nihon Dempa Kogyo Co., Ltd. Sensing device

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS477672A (en) * 1970-09-29 1972-04-24 Westinghouse Electric Corp Electrical disconnector
JPS5682411A (en) * 1979-12-11 1981-07-06 Hiromi Ogasawara Microdisplacement detector

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS477672A (en) * 1970-09-29 1972-04-24 Westinghouse Electric Corp Electrical disconnector
JPS5682411A (en) * 1979-12-11 1981-07-06 Hiromi Ogasawara Microdisplacement detector

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59217145A (en) * 1983-05-26 1984-12-07 Fujihira Kogyo Kk Total sugar amount measuring apparatus
JPH0251140B2 (en) * 1983-05-26 1990-11-06 Fujihira Kogyo Kk
JPH01282418A (en) * 1988-05-09 1989-11-14 Hitachi Ltd Piezo-electric type physical quantity detector
JPH071207B2 (en) * 1988-05-09 1995-01-11 株式会社日立製作所 Piezoelectric physical quantity detector
JPH0357932A (en) * 1989-07-27 1991-03-13 Agency Of Ind Science & Technol Crystal temperatuer sensor for cryogenic temperature
JP2000283905A (en) * 1999-03-30 2000-10-13 Noboru Koyama Multichannel qcm sensor device
JP2010503116A (en) * 2006-09-06 2010-01-28 スリーエム イノベイティブ プロパティズ カンパニー Spatially distributed remote sensors
JP2012008029A (en) * 2010-06-25 2012-01-12 Nippon Dempa Kogyo Co Ltd Sensing device
US9086338B2 (en) 2010-06-25 2015-07-21 Nihon Dempa Kogyo Co., Ltd. Sensing device

Also Published As

Publication number Publication date
JPH0245802B2 (en) 1990-10-11

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