JPH0216858B2 - - Google Patents
Info
- Publication number
- JPH0216858B2 JPH0216858B2 JP57013892A JP1389282A JPH0216858B2 JP H0216858 B2 JPH0216858 B2 JP H0216858B2 JP 57013892 A JP57013892 A JP 57013892A JP 1389282 A JP1389282 A JP 1389282A JP H0216858 B2 JPH0216858 B2 JP H0216858B2
- Authority
- JP
- Japan
- Prior art keywords
- infrared
- opposing
- transmitting
- detector
- transmitting part
- 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 - Lifetime
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
- G01J5/02—Constructional details
- G01J5/08—Optical arrangements
- G01J5/0803—Arrangements for time-dependent attenuation of radiation signals
- G01J5/0805—Means for chopping radiation
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
- G01J5/10—Radiation pyrometry, e.g. infrared or optical thermometry using electric radiation detectors
- G01J5/34—Radiation pyrometry, e.g. infrared or optical thermometry using electric radiation detectors using capacitors, e.g. pyroelectric capacitors
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
- G01N21/314—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry with comparison of measurements at specific and non-specific wavelengths
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
- G01N21/35—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Photometry And Measurement Of Optical Pulse Characteristics (AREA)
- Radiation Pyrometers (AREA)
Description
【発明の詳細な説明】 本発明は赤外線検出器に関する。[Detailed description of the invention] The present invention relates to an infrared detector.
近時の赤外線検出器では、その赤外線検出部に
例えば焦電型の赤外線検出体が内蔵されている。
斯る赤外線検出体は入射赤外線の変化量に基づい
て電荷を発生する特性を有し、又上記赤外線検出
体の検出精度は入射赤外線量の変化が周期的であ
る程向上し、従つて上記赤外線検出体に入射する
赤外線を周期的に断続する必要があり、このため
に第1図a及びbに示す如く赤外線検出器1の前
方にはモータ2によつて周期的に回転駆動される
金属板チヨツパ3が配置されている。 In recent infrared detectors, for example, a pyroelectric infrared detector is built into the infrared detector.
Such an infrared detector has a characteristic of generating electric charge based on the amount of change in the amount of incident infrared rays, and the detection accuracy of the infrared detector improves as the amount of incident infrared rays changes more periodically. It is necessary to periodically interrupt the infrared rays incident on the detection object, and for this purpose, as shown in FIG. Chiyotsupa 3 is placed.
しかし乍ら、斯るチヨツパ3は形状が大きくス
ペース上の問題があり、且つ上記モータ2は回転
むらを生じて必ずしもチヨツパ3を周期的に回転
駆動しないため検出精度の低下を招いてしまう。 However, such a chopper 3 has a large shape and there is a space problem, and the motor 2 has uneven rotation and does not necessarily rotate the chopper 3 periodically, resulting in a decrease in detection accuracy.
本発明は斯る点に鑑みてなされたもので、以下
本発明実施例を図面に基づいて詳述する。 The present invention has been made in view of these points, and embodiments of the present invention will be described in detail below with reference to the drawings.
第2図は赤外線検出器4を示し、5はタンタル
酸リチウム(LiTaO3)単結晶から成り入射赤外
線変化量に応じて電荷を発生する焦電型の赤外線
検出体、6及び7は夫々該赤外線検出体の表、裏
面にニクロム蒸着膜にて形成された表、裏面電
極、8は銅、燐青銅などからなる金属性支持台
で、該支持台上には、上記裏面電極7を支持台8
上面に対向するようにして、上記赤外線検出体5
が銀ペーストなどの導電性接着剤9にて固着され
ている。 FIG. 2 shows an infrared detector 4, in which 5 is a pyroelectric infrared detector made of lithium tantalate (LiTaO 3 ) single crystal and generates a charge according to the amount of change in incident infrared rays, and 6 and 7 are infrared ray detectors, respectively. Front and back electrodes are formed on the front and back surfaces of the detection object using nichrome vapor deposited films, and reference numeral 8 is a metal support made of copper, phosphor bronze, etc. On the support, the back electrode 7 is mounted on a support 8.
The infrared detecting body 5 is arranged so as to face the upper surface.
is fixed with a conductive adhesive 9 such as silver paste.
10は上記赤外線検出体5が高抵抗であるが故
に斯る高抵抗を低抵抗に変換するためのインピー
ダンス変換回路11が配置されたアルミナ基板、
12は金属性のキヤツプ13及びヘツダ14から
なる収納体で、該収納体内の上記ヘツダ14上に
は上記支持台8及び基板10が固定されている。
15は上記ヘツダ14に直接的に植設されたアー
ス端子で、該端子は上記支持台8及び接着剤9を
介して上記裏面電極7に電気的に接続されてい
る。16及び17は夫々上記ヘツダ14に絶縁材
18,19を介して植設された第1、第2リード
端子、20は上記表面電極6とインピーダンス変
換回路11とを結線するリード線、21,22は
上記インピーダンス変換回路11と第1、第2リ
ード端子16,17とを結線するリード線であ
る。 10 is an alumina substrate on which an impedance conversion circuit 11 is arranged to convert the high resistance of the infrared detector 5 to a low resistance because the infrared detector 5 has a high resistance;
Reference numeral 12 denotes a storage body consisting of a metal cap 13 and a header 14, and the support stand 8 and the substrate 10 are fixed on the header 14 inside the storage body.
Reference numeral 15 denotes a ground terminal directly implanted in the header 14, and the terminal is electrically connected to the back electrode 7 via the support base 8 and adhesive 9. 16 and 17 are first and second lead terminals implanted in the header 14 via insulating materials 18 and 19, respectively; 20 are lead wires connecting the surface electrode 6 and the impedance conversion circuit 11; 21 and 22; is a lead wire that connects the impedance conversion circuit 11 and the first and second lead terminals 16 and 17.
23は上記赤外線検出体5に表面電極5側から
赤外線を入射せしめるべく上記キヤツプ13に穿
設された開口、24は該開口を閉塞する第1赤外
線透過体で、該透過体は波長2〜15μmの赤外線
に対する透過率が高い厚さ数100μmのシリコン又
はゲルマニウム板からなつている。25は上記開
口23に対向すべく上記第1赤外線透過体24の
下面に固定された平面状の第1対向体(詳細は後
述する)、26は上記収納体12内において上記
第1赤外線透過体24に近接対向すべく配置され
た第2赤外線透過体で、該透過体は上記第1赤外
線透過体24と同様に波長2〜15μmの赤外線に
対する透過率が高い厚さ数100μmのシリコン又は
ゲルマニウム板からなつている。27は上記開口
23に対向すべく、更には上記第1対向体25に
平行にして近接対向すべく上記第2赤外線透過体
26の上面に固定された平面状の第2対向体(詳
細は後述する)である。 23 is an opening formed in the cap 13 to allow infrared rays to enter the infrared detector 5 from the surface electrode 5 side; 24 is a first infrared transmitting member that closes the opening; the transmitting member has a wavelength of 2 to 15 μm; It is made of a silicon or germanium plate several 100 μm thick that has high transmittance to infrared rays. 25 is a planar first opposing body fixed to the lower surface of the first infrared transmitting body 24 to face the opening 23 (details will be described later); 26 is the first infrared transmitting body in the storage body 12; 24, which is a second infrared transmitting body disposed close to and opposite to the first infrared transmitting body 24, which is a silicon or germanium plate having a thickness of several hundred μm and having a high transmittance for infrared rays having a wavelength of 2 to 15 μm. It is made up of 27 is a planar second opposing body fixed to the upper surface of the second infrared transmitting body 26 so as to face the opening 23 and further to closely oppose the first opposing body 25 in parallel with the second opposing body 27 (details will be described later). ).
28は2枚の圧電板を張り合わせて形成された
振動体、即ちバイモルフで、該バイモルフは直方
体形状を有しその長さ、幅w、厚みaは夫々約
30mm、5mm、05mmであり、水晶、ロツシエル塩、
酒石酸エチレン、ジアミン、酒石酸カリ、第一リ
ン酸カリ、第一リン酸アンモン、硫酸リチウム、
チタン酸バリウム、硫酸グリシンなどの単結晶
や、チタン酸バリウム系磁器、ジリコン酸・チタ
ン酸鉛系磁器、ニオブ酸系磁器などの磁器材料か
らなつている。そして、上記バイモルフ28は赤
外線入射方向に垂直な方向、即ち横方向に長くな
るようにして左端28′が上記ヘツダ14に設け
られた絶縁台29に固定され、右端28″に上記
第2赤外線透過体26が装着されている。30及
び31は上記ヘツダ14に絶縁材32,33を介
して植設された第3、第4リード端子、34及び
35は第3図にも示す如く上記バイモルフ28の
左端28′の両面に形成された第1、第2振動電
極で、該第1、第2振動電極は夫々上記第3、第
4リード端子30,31に接続されている。 28 is a vibrating body formed by pasting together two piezoelectric plates, that is, a bimorph, and the bimorph has a rectangular parallelepiped shape, and its length, width w, and thickness a are each about approx.
30mm, 5mm, 05mm, crystal, Lotsiel salt,
Ethylene tartrate, diamine, potassium tartrate, potassium monophosphate, ammonium monophosphate, lithium sulfate,
It is made of single crystals such as barium titanate and glycine sulfate, and porcelain materials such as barium titanate-based porcelain, zirconate/lead titanate-based porcelain, and niobate-based porcelain. The bimorph 28 is elongated in the direction perpendicular to the infrared incident direction, that is, in the lateral direction, and its left end 28' is fixed to an insulating stand 29 provided on the header 14. The body 26 is attached. Reference numerals 30 and 31 are third and fourth lead terminals implanted in the header 14 via insulating materials 32 and 33, and 34 and 35 are the bimorph 28 as shown in FIG. The first and second vibrating electrodes are formed on both sides of the left end 28', and the first and second vibrating electrodes are connected to the third and fourth lead terminals 30 and 31, respectively.
而して、上記第1、第2振動電極34,35間
に第3、第4リード端子30,31を介して所定
の交流信号を印加すると、上記バイモルフ28は
交流信号の周波数に応じて撓んで第2赤外線透過
体26を円弧状A方向(第3図)に周期的に振動
せしめる。この場合、上記2対向体27は第1対
向体25に対して常に平行状態に保持されながら
円弧状A方向に周期的に振動する。 When a predetermined AC signal is applied between the first and second vibrating electrodes 34 and 35 via the third and fourth lead terminals 30 and 31, the bimorph 28 flexes in accordance with the frequency of the AC signal. Then, the second infrared transmitting body 26 is periodically vibrated in the arcuate direction A (FIG. 3). In this case, the two opposing bodies 27 vibrate periodically in the arcuate A direction while always being held parallel to the first opposing body 25.
ここで、上記第1、第2対向体25,27を詳
述するに、第2対向体27において36,36…
はアルミニウム、金、銀などの赤外線非透過材料
からなり紙面に略平行な方向(第2図)にて第4
図bに示す如く線状に延設された複数の第2赤外
線非透過部、37,37…は該第2赤外線非透過
部の各々の間に位置し第2赤外線非透過部36,
36…と同一の形状及び寸法を有する第2赤外線
非透過部である。そして第2赤外線非透過部3
6,36…及び第2赤外線透過部37,37…の
各部分の振動方向寸法は各部分の振動幅に比例し
ている。従つて、第2対向体27は円弧状A方向
に振動するから、上記第2赤外線非透過部36,
36…及び第2赤外線透過部37,37…は共
に、上記バイモルフ28に最も近い部分の振動方
向寸法が最小幅W1となりバイモルフ28から最
も遠い部分の振動方向寸法が最大幅W2となるよ
うな扇形をなしている。 Here, to explain the first and second opposing bodies 25, 27 in detail, in the second opposing body 27, 36, 36...
is made of a material that does not transmit infrared rays, such as aluminum, gold, or silver.
As shown in FIG. b, a plurality of linearly extending second infrared non-transmissive parts 37, 37, . . . are located between the second infrared non-transparent parts 36,
This is a second infrared opaque portion having the same shape and dimensions as 36.... and a second infrared non-transmissive part 3
The dimensions in the vibration direction of each portion of the second infrared transmitting portions 37, 37, . . . are proportional to the vibration width of each portion. Therefore, since the second opposing body 27 vibrates in the arcuate direction A, the second infrared non-transmissive portion 36,
36... and the second infrared transmitting parts 37, 37... are such that the dimension in the vibration direction of the part closest to the bimorph 28 is the minimum width W1 , and the dimension in the vibration direction of the part farthest from the bimorph 28 is the maximum width W2 . It is fan-shaped.
更に、上記第1対向体25において、38,3
8…は上記第2赤外線非透過部36,36…と同
一材料からなり紙面に略平行な方向(第2図)に
て第4図aに示す如く線状に延設された複数の第
1赤外線非透過部、39,39…は該第1赤外線
非透過部の各々の間に位置する第1赤外線透過部
で、上記第1赤外線非透過部38,38…及び第
1赤外線透過部39,39…は上記第2対向体2
7の第2赤外線非透過部36,36…及び第2赤
外線透過部37,37…と同一の扇形状及び寸法
を有している。 Furthermore, in the first opposing body 25, 38,3
8... are made of the same material as the second infrared non-transmissive parts 36, 36..., and are arranged linearly in a direction substantially parallel to the paper surface (FIG. 2) as shown in FIG. 4a. The infrared opaque parts 39, 39... are first infrared transmissive parts located between the first infrared opaque parts, and the first infrared opaque parts 38, 38... 39... is the second opposing body 2
It has the same fan shape and dimensions as the second infrared non-transmissive portions 36, 36, . . . and the second infrared ray transmissive portions 37, 37, .
そして、例えば、上記第1赤外線非透過部3
8,38…、第1赤外線透過部39,39…、第
2赤外線非透過部36,36…及び第2赤外線透
過部37,37…の幅W1,W2は夫々100μm、
120μmであり長さは3mm、厚さDは0.1〜
100μmである。 For example, the first infrared non-transmissive portion 3
8, 38..., the first infrared transmitting parts 39, 39..., the second infrared non-transmitting parts 36, 36, and the second infrared transmitting parts 37, 37... have widths W 1 and W 2 of 100 μm, respectively.
120μm, length is 3mm, thickness D is 0.1~
It is 100μm.
而して、上記バイモルフ28の振動時には、上
記第2対向体27の第2赤外線非透過部36,3
6…は第5図に詳細に示す如く上記第1対向体2
5の第1赤外線非透過部38,38…及び第1赤
外線透過部39,39…に交互に完全に重畳する
ように、即ち打点領域I及び斜線領域Jに位置す
るように振動する。 Therefore, when the bimorph 28 vibrates, the second infrared non-transmissive portions 36, 3 of the second opposing body 27
6... is the first opposing body 2 as shown in detail in FIG.
It vibrates so as to alternately and completely overlap the first infrared non-transmissive parts 38, 38, . . . and the first infrared ray transmissive parts 39, 39, .
ここに、上記第1赤外線非透過部38,39
…、第1赤外線透過部39,39…、第2赤外線
非透過部36,36…及び第2赤外線透過部3
7,37…の幅は第6図a,bに示す如く一定と
するのが通常である。この場合、第2対向体27
は円弧状A方向に振動するから、例えば第2赤外
線非透過部36,36…は第7図に示す如く第1
赤外線非透過部38,38…に完全には重畳しな
い。すると、赤外線検出器4外部の被検出体から
の赤外線を周期的に断続して赤外線検出体5に入
射する赤外線を周期的に変化せしめるにも、即ち
交流的に変調せしめるにもその変調度が悪く、従
つて赤外線検出体5におけるSN比が低下してし
まう。 Here, the first infrared non-transmissive portions 38, 39
..., first infrared transmitting sections 39, 39..., second infrared non-transmitting sections 36, 36..., and second infrared transmitting section 3
The widths of 7, 37, . . . are usually constant as shown in FIGS. 6a and 6b. In this case, the second opposing body 27
vibrates in the arc-shaped direction A, so for example, the second infrared non-transmissive portions 36, 36...
It does not completely overlap with the infrared opaque parts 38, 38, . . . Then, even if the infrared rays from the object to be detected outside the infrared detector 4 are periodically interrupted and the infrared rays incident on the infrared detector 5 are changed periodically, that is, the infrared rays are modulated in an alternating current manner, the degree of modulation will be different. Therefore, the SN ratio of the infrared detector 5 decreases.
この点、上記赤外線検出器4では、第2赤外線
非透過部36,36…は第1赤外線非透過部3
8,38…及び第1赤外線透過部39,39…に
完全に重畳するから、赤外線検出体5に入射する
赤外線の変調度は良好であり、従つて赤外線検出
体5におけるSN比は顕著に向上する。尚、赤外
線検出体5の出力は被検出体の温度と室温との温
度差に基づいている。 In this regard, in the infrared detector 4, the second infrared non-transmissive portions 36, 36, . . .
8, 38... and the first infrared transmitting parts 39, 39..., the degree of modulation of the infrared rays incident on the infrared detector 5 is good, and therefore the SN ratio in the infrared detector 5 is significantly improved. do. Note that the output of the infrared detector 5 is based on the temperature difference between the temperature of the object to be detected and the room temperature.
第8図は上記赤外線検出器4を含む回路を示
し、赤外線検出器4内のインピーダンス変換回路
11は1010〜1011Ωの高入力抵抗40、FET(電界
効果トランジスタ)41及び約10KΩの出力抵抗
42にて形成されている。 FIG. 8 shows a circuit including the infrared detector 4, and the impedance conversion circuit 11 in the infrared detector 4 has a high input resistance 40 of 10 10 to 10 11 Ω, an FET (field effect transistor) 41, and an output of about 10 KΩ. It is formed of a resistor 42.
そして、上記赤外線検出器4は第1リード端子
16にて直流電圧が供給され、第2リード端子1
7から被検出体の温度と室温との温度差に応じた
交流信号が出力される。43は室温測定を行なう
ダイオード、44は無安定マルチバイブレータか
らなり周期的パルスを発振する発振器、45は上
記パルスに基づいて上記バイモルフ28を振動せ
しめる(撓ませる)ための交流信号を出力する駆
動回路、46,47,48は直流増幅器、49は
フイルタ増幅器、50は周期検波器で、上記赤外
線検出器4からの交流信号と上記発振器44から
のパルスとの同期をとり、被検出体の温度が室温
より高い場合はその温度差に応じた正の直流信号
を出力し、被検出体の温度が室温より低い場合は
その温度差に応じた負の直流信号を出力する。5
1は上記同期検波器50の出力とダイオード43
の出力とを合成(加算)する合成回路で、該回路
は被検出体の温度に応じた信号を出力する。52
は斯る温度を所望回路へ出力するための出力端子
である。 The infrared detector 4 is supplied with a DC voltage at a first lead terminal 16, and a second lead terminal 1
7 outputs an AC signal corresponding to the temperature difference between the temperature of the object to be detected and the room temperature. 43 is a diode for measuring room temperature; 44 is an oscillator made of an astable multivibrator that oscillates periodic pulses; and 45 is a drive circuit that outputs an alternating current signal to vibrate (deflect) the bimorph 28 based on the pulses. , 46, 47, and 48 are DC amplifiers, 49 is a filter amplifier, and 50 is a periodic detector, which synchronizes the AC signal from the infrared detector 4 with the pulse from the oscillator 44, and adjusts the temperature of the object to be detected. If the temperature of the object to be detected is higher than room temperature, a positive DC signal corresponding to the temperature difference is output, and if the temperature of the object to be detected is lower than room temperature, a negative DC signal corresponding to the temperature difference is output. 5
1 is the output of the synchronous detector 50 and the diode 43
This circuit outputs a signal corresponding to the temperature of the object to be detected. 52
is an output terminal for outputting the temperature to a desired circuit.
以上の説明から明らかな如く、本発明によれば
入射赤外線変化量に応じて電荷を発生する赤外線
検出体、該検出体を収納する収納体、被検出体か
らの赤外線を上記赤外線検出体へ入射せしめるべ
く上記収納体に穿設された開口、赤外線透過部及
び赤外線非透過部を共に有し互いに平行にして上
記開口に対向すべく配置された平面状の一対の対
向体、長手方向に対して垂直に自由に振動可能な
自由開放端の先端部に一方の前記対向体を装着し
且つ上記平行状態を保持しながら一方の対向体を
その赤外線非透過部が他方の対向体の赤外線透過
部及び赤外線非透過部に周期的に交互に重畳する
ように振動せしめる振動体を備え、上記一方の対
向体の赤外線透過部及び赤外線非透過部におい
て、その形状及び寸法は互いに同一とし、各部分
の振動方向の寸法は各部分の振動幅に比例せし
め、更に上記他方の対向体の赤外線透過部及び赤
外線非透過部の形状及び寸法は上記一方の対向体
の赤外線透過部及び赤外線非透過部と同一とした
から、従来の如きチヨツパ及びモータが不要とな
り、従つて赤外線検出部を小型化できると共に、
赤外線検出体に入射する赤外線はむらなく周期的
に変化するため高精度の下に赤外線検出を行なう
ことができる。更に、赤外線を変化せしめる場合
の変調度を向上でき、従つて赤外線検出体におけ
るSN比を顕著に向上できる。 As is clear from the above description, according to the present invention, there is an infrared detector that generates a charge according to the amount of change in incident infrared radiation, a storage body that stores the detector, and an infrared ray from a detected object that is incident on the infrared detector. a pair of planar opposing bodies having both an infrared transmitting part and an infrared non-transmitting part and disposed parallel to each other to face the opening, with respect to the longitudinal direction; One of the opposing bodies is attached to the tip of the free open end that can freely vibrate vertically, and while maintaining the above-mentioned parallel state, the infrared non-transmitting part of one of the opposing bodies is connected to the infrared transmitting part of the other opposing body. The infrared transmissive part and the infrared non-transmissive part of one opposing body have the same shape and dimensions, and the vibration of each part is The dimension in the direction is proportional to the vibration width of each part, and the shape and dimensions of the infrared transmitting part and the infrared non-transmitting part of the other opposing body are the same as the infrared transmitting part and the infrared non-transmitting part of the one opposing body. Therefore, the conventional tipper and motor are no longer necessary, and the infrared detection section can be made smaller.
Since the infrared rays incident on the infrared detector vary evenly and periodically, infrared rays can be detected with high precision. Furthermore, the degree of modulation when changing infrared rays can be improved, and therefore the SN ratio of the infrared detector can be significantly improved.
また、特開昭56−160628号(G01J、5/62)
に記載の従来技術においては圧電振動子の伸び方
向(縦方向)の振動を用いているが、伸び方向の
振幅量は100Vの印加でもせいぜい10μm程度であ
る。一方、本発明においてはバイモルフ振動子の
横方向の振幅量を利用しているので、数10Vの印
加でも数10μmの大きな振幅、即ち、前者に比較
して約10倍の振幅量を得ることができ、極めて効
率がよい。また、この従来例においては2個の発
振器を要し、而も両発器の発振周波数の差の周波
数で赤外線をチヨツピングするので、その周波数
を精度よく制御する必要があるが、本発明ではそ
のような高精度の発振器を要せず、而も1個で事
足りる。 Also, JP-A-56-160628 (G01J, 5/62)
The prior art described in 1 uses vibration in the elongation direction (vertical direction) of the piezoelectric vibrator, but the amplitude in the elongation direction is at most about 10 μm even when 100V is applied. On the other hand, in the present invention, since the lateral amplitude of the bimorph oscillator is utilized, it is possible to obtain a large amplitude of several tens of μm even when applying several tens of V, that is, an amplitude approximately ten times as large as that of the former. possible and extremely efficient. In addition, in this conventional example, two oscillators are required, and since the infrared rays are stepped at a frequency that is the difference between the oscillation frequencies of both oscillators, it is necessary to precisely control the frequency. There is no need for such a high-precision oscillator; even one is sufficient.
また、特開昭56−128432号(G01J 1/42)に
示されている技術においては、回転円板上の光透
過部の寸法を振動幅に比例するようにした例が示
されているが、この従来例では1枚の回転円板を
モーターで回転駆動するに過ぎない。また、特開
昭55−54418号(G01J 5/14)第5図にはバイ
モルフを使用して光を断続する例が示されている
が、本発明で述べた如き構成および効果を有する
ものではない。 Furthermore, in the technique shown in Japanese Patent Application Laid-Open No. 56-128432 (G01J 1/42), an example is shown in which the dimensions of the light transmitting part on the rotating disk are made proportional to the vibration width. In this conventional example, only one rotary disk is rotated by a motor. Further, Fig. 5 of Japanese Patent Application Laid-Open No. 55-54418 (G01J 5/14) shows an example of intermittent light using a bimorph, but this does not have the structure and effect as described in the present invention. do not have.
第1図a及びbは夫々従来の赤外線検出機構の
側面図及び平面図、第2図は本発明実施例赤外線
検出器の断面図、第3図は第2図において矢印
方向から見た図、第4図a,bは夫々同要部平面
図、第5図は同要部の動作状態図、第6図a,b
は夫々第4図a,bに対応する赤外線検出器の一
般的要部平面図、第7図は同要部の動作状態図、
第8図は第2図の赤外線検出器を含む回路図であ
る。
5……赤外線検出体、12……収納体、23…
…開口、25……第1対向体、38,38……第
1赤外線非透過部、39,39……第1赤外線透
過部、27……第2対向体、36,36……第2
赤外線非透過部、37,37……第2赤外線透過
部、28……バイモルフ。
1A and 1B are a side view and a plan view of a conventional infrared detection mechanism, FIG. 2 is a sectional view of an infrared detector according to an embodiment of the present invention, and FIG. 3 is a view seen from the direction of the arrow in FIG. Figures 4a and b are plan views of the same essential parts, Figure 5 is a diagram of the operating state of the same parts, and Figures 6a and b.
are general plan views of the main parts of the infrared detector corresponding to Figs. 4a and b, respectively, and Fig. 7 is a diagram of the operating state of the same main parts,
FIG. 8 is a circuit diagram including the infrared detector of FIG. 2. 5... Infrared detector, 12... Storage body, 23...
...opening, 25...first opposing body, 38, 38...first infrared non-transmissive section, 39, 39...first infrared transmitting section, 27...second opposing body, 36, 36...second
Infrared non-transmissive part, 37, 37...Second infrared transmissive part, 28...Bimorph.
Claims (1)
外線検出体5と、該検出体を収納する収納体12
と、被検出体からの赤外線を前記赤外線検出体へ
入射せしめるべく前記収納体に穿設された開口2
3と、赤外線透過部39及び赤外線非透過部38
を共に有し互いに平行にして前記開口23に対向
すべく配置された平面状の一対の対向体25,2
7と、長手方向に対して垂直に自由に振動可能な
自由開放端の先端部に一方の前記対向体を装着し
且つ前記平行状態を保持しながら前記一方の対向
体をその赤外線非透過部が他方の対向体の赤外線
透過部及び赤外線非透過部に周期的に交互に重畳
するように振動せしめるバイモルフ振動体28と
を備え、前記一方の対向体の赤外線透過部及び赤
外線非透過部において、その形状及び寸法は互い
に同一とし、各部分の振動方向の寸法は各部分の
振動幅に比例せしめ、更に、上記他方の対向体の
赤外線透過部及び赤外線非透過部の形状及び寸法
は上記一方の対向体の赤外線透過部及び赤外線非
透過部と同一にしてなる赤外線検出器。1. An infrared detector 5 that generates a charge according to the amount of change in incident infrared rays, and a storage body 12 that stores the detector.
and an opening 2 formed in the housing to allow infrared rays from the object to be detected to enter the infrared detecting object.
3, an infrared transmitting section 39 and an infrared non-transmitting section 38
a pair of planar opposing bodies 25, 2 that are parallel to each other and are arranged to face the opening 23;
7, one of the opposing bodies is attached to the tip of the free open end that can freely vibrate perpendicularly to the longitudinal direction, and while maintaining the parallel state, the one of the opposing bodies is attached so that its infrared non-transmissive part is a bimorph vibrating body 28 that vibrates so as to be periodically and alternately superimposed on the infrared transmitting part and the infrared non-transmitting part of the one opposing body; The shapes and dimensions are the same, the dimensions in the vibration direction of each part are proportional to the vibration amplitude of each part, and the shapes and dimensions of the infrared transmitting part and the infrared non-transmitting part of the other opposing body are the same as that of the one opposing body. An infrared detector consisting of an infrared transmitting part and an infrared non-transmitting part of the body.
Priority Applications (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57013892A JPS58129334A (en) | 1982-01-29 | 1982-01-29 | infrared detector |
| US06/407,582 US4485305A (en) | 1981-08-20 | 1982-08-12 | Infrared detector with vibrating chopper |
| GB08223932A GB2105033B (en) | 1981-08-20 | 1982-08-19 | Infrared ray detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57013892A JPS58129334A (en) | 1982-01-29 | 1982-01-29 | infrared detector |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58129334A JPS58129334A (en) | 1983-08-02 |
| JPH0216858B2 true JPH0216858B2 (en) | 1990-04-18 |
Family
ID=11845829
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57013892A Granted JPS58129334A (en) | 1981-08-20 | 1982-01-29 | infrared detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58129334A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6118887A (en) * | 1984-07-06 | 1986-01-27 | Yokogawa Hokushin Electric Corp | Chopper |
| US5019710A (en) * | 1989-03-30 | 1991-05-28 | Measurex Corporation | Optical system for detecting properties of traveling sheet materials |
Family Cites Families (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS56128432A (en) * | 1980-03-13 | 1981-10-07 | Brother Ind Ltd | Optical detector |
| JPS56160628A (en) * | 1980-05-14 | 1981-12-10 | Sanyo Electric Co Ltd | Infrared detector |
| JPS5711518A (en) * | 1980-06-24 | 1982-01-21 | Citizen Watch Co Ltd | Manufacture for tuning fork type quartz oscillator |
| JPS5798033U (en) * | 1980-12-05 | 1982-06-16 |
-
1982
- 1982-01-29 JP JP57013892A patent/JPS58129334A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58129334A (en) | 1983-08-02 |
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