JPH01260366A - Space filter type speed detector - Google Patents

Space filter type speed detector

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Publication number
JPH01260366A
JPH01260366A JP8816388A JP8816388A JPH01260366A JP H01260366 A JPH01260366 A JP H01260366A JP 8816388 A JP8816388 A JP 8816388A JP 8816388 A JP8816388 A JP 8816388A JP H01260366 A JPH01260366 A JP H01260366A
Authority
JP
Japan
Prior art keywords
light
spatial filter
measured
speed detection
light source
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
JP8816388A
Other languages
Japanese (ja)
Inventor
Shigeki Tsuchiya
茂樹 土谷
Masahiro Matsumoto
昌大 松本
Kiyomitsu Suzuki
清光 鈴木
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
Original Assignee
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 Ltd filed Critical Hitachi Ltd
Priority to JP8816388A priority Critical patent/JPH01260366A/en
Publication of JPH01260366A publication Critical patent/JPH01260366A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To enable stable highly accurate detection of speed under varied conditions, by providing a space filter with a wavelength selecting means to remove effect of extraneous light on the speed detection. CONSTITUTION:An infrared monochromatic ray with a specified wavelength band is irradiated to a measuring field of view of an object 7 to be measured such as a road surface from a light emitting diode 2. A reflection optical image of the infrared monochromatic ray corresponding to the measuring field of view is focused onto a space filter detector 4 with an objective lens 1 through an interference filter 3, which has a pass area somewhat broader than a half width of a radiation spectrum centered on the center wavelength of the light emitting diode 2. An output of the space filter detector 4 is applied to a signal processing circuit 6 through a pre-amplifier 5.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、被測定物との相対速度を空間フィルタ方式に
より、非接触で光学的に検出するようにした速度検出装
置に係り、特に外来光の影響を受けずに高精度の速度測
定を行なう空間フィルタ式速度検出装置に関する。
Detailed Description of the Invention [Industrial Application Field] The present invention relates to a speed detection device that optically detects the relative speed to an object to be measured in a non-contact manner using a spatial filter method. The present invention relates to a spatial filter speed detection device that measures speed with high precision without being affected by light.

[従来の技術] 車両の速度検出手段としては、車輪の回転速度を検出し
て行なう方式のものが主に用いられていたが、アンチス
キッド制御などを考慮した場合、車輪の回転によらずに
速度を検出することが必要となり、たとえば、センサ技
術;vol 6. No 7(1986) p p 6
2〜67に記載されている空間フィルタ式速度検出装置
が注目されるようになっている。
[Prior Art] As a vehicle speed detection means, a method that detects the rotational speed of the wheels has mainly been used, but when considering anti-skid control etc., it is possible to detect the rotational speed of the wheels. It becomes necessary to detect speed, for example sensor technology; vol 6. No 7 (1986) p p 6
The spatial filter type speed detection devices described in Nos. 2 to 67 are attracting attention.

第3図はこの従来の空間フィルタ式速度検出装置の構成
を示し、走行路面などの被測定物7の表面を、光g8か
らの光で照射し被測定物7の光学像が、レンズ1によっ
て空間フィルタ検出器4上に集束されるようになってい
る。
FIG. 3 shows the configuration of this conventional spatial filter type speed detection device, in which the surface of the object 7 to be measured, such as a running road surface, is irradiated with light from light g8, and an optical image of the object 7 to be measured is formed by the lens 1. It is adapted to be focused onto a spatial filter detector 4.

そして、この空間フィルタ検出器4の検出信号が、プリ
アンプ5で増幅され信号処理回路6で信号処理されるこ
とにより、被測定物7との相対速度が検出されるように
なっている。
The detection signal from the spatial filter detector 4 is amplified by the preamplifier 5 and processed by the signal processing circuit 6, so that the relative velocity with respect to the object to be measured 7 is detected.

前述の空間フィルタ検出器4は、第4図に示すような構
成となっていて、シリコン太陽電池の表面に受光部10
が短冊状パターンとして形成され。
The above-mentioned spatial filter detector 4 has a configuration as shown in FIG. 4, and has a light receiving section 10 on the surface of a silicon solar cell.
is formed as a strip pattern.

これらの受光部10はSi基盤9の表面に、2組のくし
歯状パターンが互いに噛み合ったいわゆるインターディ
ジタル形状となっている。
These light receiving sections 10 have a so-called interdigital shape in which two sets of comb-like patterns are interlocked with each other on the surface of the Si substrate 9.

このように、Si基盤9に設けられる共通リード線14
とそれぞれ隣接して配される受光部1゜に接続されるリ
ード線12.13間に、独立にフォトダイオードがそれ
ぞれ形成されている。従って、光電変換信号はリード線
12.13と共通リード線14との間にそれぞれ得られ
るようになっている。
In this way, the common lead wire 14 provided on the Si substrate 9
Photodiodes are formed independently between lead wires 12 and 13 connected to the light receiving portions 1° arranged adjacent to each other. Therefore, photoelectric conversion signals are obtained between the lead wires 12 and 13 and the common lead wire 14, respectively.

このような構成の空間フィルタ式速度検出装置に対して
、被測定物7が移動すると、それにつれて空間フィルタ
検出器4上の像も移動する。そして、被測定物7の表面
の光学的明暗分布によって、リード線12.13の検出
信号に時間的変化が現われ、被測定物7の光学像の移動
に対応した周波数で変動する信号が得られる。
When the object to be measured 7 moves with respect to the spatial filter type speed detection device having such a configuration, the image on the spatial filter detector 4 also moves accordingly. Then, depending on the optical brightness distribution on the surface of the object to be measured 7, a temporal change appears in the detection signal of the lead wires 12 and 13, and a signal that fluctuates at a frequency corresponding to the movement of the optical image of the object to be measured 7 is obtained. .

光学系による被測定物の光学像の投影倍率をM。The projection magnification of the optical image of the object to be measured by the optical system is M.

受光部の配列ピッチをPとすると、ここで得られる信号
の周波数fは次式で与えられる。
When the arrangement pitch of the light receiving sections is P, the frequency f of the signal obtained here is given by the following equation.

f=MV/P          ・・・・・・(1)
そして従来は、光源8としてハロゲンランプのように可
視光領域で広い発光スペクトルを有するものが使用され
、この可視光領域に高い受光感度を有する空間フィルタ
検出器4で信号の検出が行なわれていた。
f=MV/P...(1)
Conventionally, a halogen lamp having a wide emission spectrum in the visible light region is used as the light source 8, and the signal is detected by the spatial filter detector 4, which has high light reception sensitivity in the visible light region. .

[発明が解決しようとする課題] この種の速度検出装置は、多くの場合被測定物を照射す
る光源の光重外の外来光が存在する状態で使用される。
[Problems to be Solved by the Invention] This type of speed detection device is often used in the presence of extraneous light other than the light intensity of the light source that illuminates the object to be measured.

このため、外来光が速度検出装置での速度検出に次のよ
うな悪影響を及ぼす。
Therefore, the extraneous light has the following adverse effect on speed detection by the speed detection device.

第1に、外来光の強度の時間的或は場所的変動が大きく
、この外来光の強度変動によって空間フィルタ検出器の
検出電流が大幅に変動してしまう。
First, the intensity of the extraneous light varies greatly over time or location, and the detected current of the spatial filter detector varies significantly due to the variation in the intensity of the extraneous light.

例えば、速度検出装置を昼間太陽光の下で使用した場合
と夜間使用した場合とでは、被測定物を照射する光の強
度は2桁近く異なる。また、速度検出装置を日向で使用
する場合と、日陰で使用する場合でも被測定物を照射す
る光の強度には大きな差がある。
For example, the intensity of the light irradiating the object to be measured differs by nearly two orders of magnitude when the speed detection device is used under sunlight during the day and when it is used at night. Furthermore, there is a large difference in the intensity of light irradiating the object to be measured, whether the speed detection device is used in the sun or in the shade.

このように、被測定物を照射する光の強度が大幅に変動
すると、空間フィルタ検出器に接続されるプリアンプ及
び信号処理回路が、空間フィルタ検出器の検出電流の大
きな変動に追従出来なくなり動作不能におちいることが
ある。
In this way, if the intensity of the light that illuminates the object to be measured fluctuates significantly, the preamplifier and signal processing circuit connected to the spatial filter detector will be unable to follow the large fluctuations in the detection current of the spatial filter detector and will become inoperable. I sometimes fall into this situation.

第2に、被測定物の測定視野以外の場所での外来光の反
射光が、迷光として空間フィルタ検出器に入射し、速度
検出装置の検出値が変化することがある。第5図は、こ
の場合の外来光による反射光の空間フィルタ検出器4へ
の入射を示す図で。
Second, reflected light of external light at a location other than the measurement field of the object to be measured may enter the spatial filter detector as stray light, and the detected value of the speed detection device may change. FIG. 5 is a diagram showing the incidence of reflected light from external light on the spatial filter detector 4 in this case.

同図に示すように外来光15は、被測定物7の測定視野
以外の場所で反射し、さらに速度検出装置の内壁で反射
して迷光として空間フィルタ検出器4に入射している。
As shown in the figure, the external light 15 is reflected at a location other than the measurement field of view of the object to be measured 7, further reflected by the inner wall of the speed detection device, and is incident on the spatial filter detector 4 as stray light.

このような迷光が、空間フィルタ検出器4上に作る光学
的明暗のむらは、多くの低空間周波数成分を含むので、
特に低速時における速度測定に悪影響を及ぼす。
Since the optical brightness unevenness created by such stray light on the spatial filter detector 4 includes many low spatial frequency components,
This adversely affects speed measurements, especially at low speeds.

第3に、外来光により形成される影が被測定物の測定視
野を通過して、速度検出装置の検出値が変化することが
ある。例えば、速度検出装置を搭載した車両が、太陽光
などの強い外来光で照射されると、車両の一部などの影
が被測定物の測定視野内に形成され、この影が車両の移
動によって測定視野内を通過し、速度検出装置がこの影
の速度を検出してしまうことがある。同様のことは、近
くを通過する他の物体の外来光による影が、速度検出装
置の被測定物の測定視野を通過する場合にも生じること
がある。
Third, a shadow formed by external light may pass through the measurement field of view of the object to be measured, and the detected value of the speed detection device may change. For example, if a vehicle equipped with a speed detection device is illuminated by strong external light such as sunlight, a shadow of a part of the vehicle will be formed within the measurement field of view of the object to be measured, and this shadow will be affected by the movement of the vehicle. The shadow may pass within the measurement field of view and the speed detection device may detect the speed of this shadow. A similar problem may occur when a shadow caused by extraneous light from another object passing nearby passes through the measurement field of view of the object to be measured by the speed detection device.

このような、外来光による形成される影の影響は、特に
低速度の検出時に大きく現われる。
The influence of shadows formed by extraneous light is particularly noticeable when detecting low speeds.

第4に、被測定物の測定視野内に存在する透明で滑らか
な表面を有し空気より屈折率が大きい異物質に対して、
外来光がこの物質の表面で反射して生じる迷光により検
出のSN比が低下することがある。
Fourthly, regarding foreign substances that have a transparent, smooth surface and a higher refractive index than air that exists within the measurement field of the object to be measured,
The detection signal-to-noise ratio may be reduced due to stray light generated by reflection of external light on the surface of this material.

第6図は外来光15が異物質11の表面で反射し、空間
フィルタ検出器4に迷光として入射する状態を示すもの
で、このような異物質11としては、例えば被測定物7
である路面に存在する水たまりがある。この水たまりが
外来光15である太陽光で照射されると、水たまりの内
部或は底部で乱反射される光よりも、水たまり表面から
の反射光の強度が大きくなる。
FIG. 6 shows a state in which extraneous light 15 is reflected on the surface of a foreign substance 11 and enters the spatial filter detector 4 as stray light.
There is a puddle that exists on the road surface. When this puddle is irradiated with sunlight, which is the external light 15, the intensity of the light reflected from the surface of the puddle becomes greater than the light diffusely reflected inside or at the bottom of the puddle.

このために、水たまりの底部からの反射光である検出光
に、この表面反射光が混入されて空間フィルタ検出器4
に入射するのでSN比が低下し、場合によっては速度検
出が不可能となることもある。
For this reason, this surface reflected light is mixed into the detection light that is the reflected light from the bottom of the puddle, and the spatial filter detector 4
Since the light is incident on the ground, the signal-to-noise ratio decreases, and in some cases, speed detection may become impossible.

本発明は、前述したような空間フィルタ式速度検出装置
の現状に基づいてなされたものであり、その目的は外来
光が速度検出に及ぼす悪影響を取り除き、各種の条件下
で常に安定した高精度の速度検出を行なう空間フィルタ
式速度検出装置を提供することにある。
The present invention has been made based on the current state of the spatial filter type speed detection device as described above, and its purpose is to eliminate the adverse effects of external light on speed detection, and to provide stable and highly accurate speed detection under various conditions. An object of the present invention is to provide a spatial filter type speed detection device that performs speed detection.

[課題を解決するための手段] 前記目的は、被測定物を照射する光源として所定波長帯
域の光を照射する光源を使用し、空間フィルタに波長選
択手段を設け、この波長選択手段により空間フィルタ検
出器に、前記光源の波長帯域の光学像のみを集束するよ
うにして達成される。
[Means for Solving the Problem] The above object is to use a light source that irradiates light in a predetermined wavelength band as a light source for irradiating the object to be measured, provide a wavelength selection means in the spatial filter, and use the wavelength selection means to control the spatial filter. This is accomplished by focusing only the optical image of the wavelength band of the light source on the detector.

[作用] 本発明では、光源から被測定物の測定視野に所定波長帯
域の光(例えば赤外単色光)が照射され、測定視野から
の反射光が結像光学系で、空間フィルタ検出器上に集束
されるが、空間フィルタに設けた波長選択手段によって
、前記光源の波長帯域の光学像のみが空間フィルタ検出
器上に集束される。
[Function] In the present invention, light in a predetermined wavelength band (for example, infrared monochromatic light) is irradiated from a light source to the measurement field of the object to be measured, and the reflected light from the measurement field is reflected onto the spatial filter detector by the imaging optical system. However, only the optical image of the wavelength band of the light source is focused onto the spatial filter detector by the wavelength selection means provided in the spatial filter.

このようにして、光源によって所定波長帯域の光が、被
測定物の測定視野に照射され、波長選択手段によって前
記所定波長帯域の被測定物の反射光学像が、空間フィル
タ検出器上に集束されるので、前記所定波長帯域とは異
なる波長帯域の外来光の強度変動の影響のない安定した
速度検出が行なわれる。また、外来光に基づく迷光や外
来光で生じる影の成分の空間フィルタ検出器への入射も
波長選択手段で阻止され、誤検出がなく高精度の検出が
行なわれる。
In this way, the light source irradiates the measurement field of the object with a predetermined wavelength band, and the wavelength selection means focuses the reflected optical image of the object in the predetermined wavelength band onto the spatial filter detector. Therefore, stable speed detection is performed without being affected by intensity fluctuations of external light in a wavelength band different from the predetermined wavelength band. Further, the wavelength selection means also prevents stray light based on external light and shadow components caused by external light from entering the spatial filter detector, and highly accurate detection is performed without false detection.

さらに、光源の照射光の波長と被測定物の測定視野に対
する入射角を選択することにより、被測定物上に存在す
る異物質(例えば路面上の水たまり)表面での反射光を
減少させ、常に高感度での速度検出が行なわれる。
Furthermore, by selecting the wavelength of the irradiated light from the light source and the angle of incidence with respect to the measurement field of view of the object to be measured, light reflected from the surface of foreign substances (for example, puddles on the road surface) existing on the object to be measured can be reduced, and the Speed detection is performed with high sensitivity.

[実施例] 以下、本発明の実施例を図面を用いて詳細に説明する。[Example] Embodiments of the present invention will be described in detail below with reference to the drawings.

第1図は本発明の実施例の構成を示す説明図で。FIG. 1 is an explanatory diagram showing the configuration of an embodiment of the present invention.

すでに従来の空間フィルタ式速度検出装置の説明に使用
した第2図と、同一部分には同一符号が付されている。
The same parts are given the same reference numerals as in FIG. 2, which has already been used to explain the conventional spatial filter type speed detection device.

第1図に示すように、筐体17の開口端側に赤外単色光
の発光ダイオード2が取り付けられており、この発光ダ
イオード2は外来光の放射スペクトル成分の強度が低い
スペクトル特性を有し、その発光強度は50mWと比較
的高い発光強度に選択されている。筐体17の開口端を
塞ぐようにして、対物レンズ1が取り付けられ、この対
物レンズ1によって被測定物7の測定視野の光学像が、
空間フィルタ検出器4上に集束するようになっている。
As shown in FIG. 1, an infrared monochromatic light emitting diode 2 is attached to the open end side of the housing 17, and this light emitting diode 2 has a spectral characteristic in which the intensity of the radiation spectrum component of external light is low. , its emission intensity is selected to be relatively high at 50 mW. An objective lens 1 is attached so as to close the opening end of the housing 17, and an optical image of the measurement field of the object to be measured 7 is formed by the objective lens 1.
It is adapted to be focused onto a spatial filter detector 4.

この空間フィルタ検出器4は、可視光帯域及び赤外光帯
域に受光感度を有する例えばシリコン太陽電池を使用し
た空間フィルタ検出器である。前述の発光ダイオード2
の発光波長は、この空間フィルタ検出器4の受光感度の
大きな波長に選定されている。
This spatial filter detector 4 is a spatial filter detector that uses, for example, a silicon solar cell and has light receiving sensitivity in the visible light band and infrared light band. The aforementioned light emitting diode 2
The emission wavelength is selected to be a wavelength at which the spatial filter detector 4 has a high light receiving sensitivity.

筐体17内において、この空間フィルタ検出器4と対物
レンズ1間に干渉フィルタ3が配設されている。第2図
は実施例の動作特性を示す波長と放射スペクトル強度及
び透過率間の特性図であり、同図に示すように、前記干
渉フィルタ3の透過率が最大の波長は、発光ダイオード
2の放射スペクトル強度が最大の中心波長近傍に設定さ
れている。
In the housing 17, an interference filter 3 is disposed between the spatial filter detector 4 and the objective lens 1. FIG. 2 is a characteristic diagram showing the operating characteristics of the embodiment between wavelength, radiation spectrum intensity, and transmittance. As shown in the figure, the wavelength at which the transmittance of the interference filter 3 is maximum is the wavelength of the light emitting diode 2 The radiation spectrum intensity is set near the center wavelength where it is maximum.

そして、干渉フィルタ3の通過域の半値幅は、発光ダイ
オード2の放射スペクトルの半値幅よりやや広い値とな
るように設定されている。
The half-width of the passband of the interference filter 3 is set to be slightly wider than the half-width of the radiation spectrum of the light-emitting diode 2.

実施例のその他の部分の構成は、すでに第3図を用いて
説明した従来の空間フィルタ式速度検出装置と同一であ
る。
The configuration of other parts of the embodiment is the same as the conventional spatial filter type speed detection device already explained using FIG.

このような構成の実施例において1発光ダイオード2が
光源を、対物レンズ1が結像光学系を、干渉フィルタ3
が波長選択手段を、それぞれ構成している。
In an embodiment with such a configuration, 1 light emitting diode 2 serves as a light source, objective lens 1 serves as an imaging optical system, and interference filter 3 serves as a light source.
constitute the wavelength selection means.

次に実施例の動作を説明する。Next, the operation of the embodiment will be explained.

実施例においては、発光ダイオード2から中心波長がほ
ぼ0.9μmの赤外単色光が、路面などの被測定物7の
測定視野に照射される。この測定視野に対応する赤外単
色光の反射光学像は、対物レンズ1によって干渉フィル
タ3を介して空間フィルタ検出器4上に集束される。
In the embodiment, monochromatic infrared light having a center wavelength of approximately 0.9 μm is irradiated from the light emitting diode 2 onto the measurement field of view of the object to be measured 7 such as a road surface. A reflected optical image of monochromatic infrared light corresponding to this measurement field of view is focused by the objective lens 1 via the interference filter 3 onto the spatial filter detector 4 .

対物レンズ1と空間フィルタ検出器4間に配されている
干渉フィルタ3は、第2図に示すように発光ダイオード
2の放射スペクトルの中心波長を中心に、この放射スペ
クトルの半値幅よりもやや広い通過域を有するので1発
光ダイオード2の赤外単色光以外の波長の光が直接或は
被測定物7表面で反射して、空間フィルタ検出器4に達
することは殆どなくなる。
The interference filter 3 disposed between the objective lens 1 and the spatial filter detector 4 has a width slightly wider than the half-value width of the emission spectrum of the light emitting diode 2, centered on the center wavelength of the emission spectrum, as shown in Fig. 2. Since it has a passband, light of wavelengths other than the infrared monochromatic light of one light emitting diode 2 is almost never reflected directly or by the surface of the object to be measured 7 and reaches the spatial filter detector 4 .

また、被測定物7が路面の場合に路面上に存在する水た
まりの表面で、発光ダイオード2からの放射光が反射し
たいように、発光ダイオード2からの放射光の路面への
入射角を設定することが簡単に行なえるので、水たまり
が存在してもSN比が低下せず高感度の速度検出が行な
われる。
Further, when the object to be measured 7 is a road surface, the incident angle of the light emitted from the light emitting diode 2 to the road surface is set so that the light emitted from the light emitting diode 2 is desired to be reflected on the surface of a puddle existing on the road surface. This can be done easily, so even if there is a puddle, the S/N ratio will not decrease and highly sensitive speed detection can be performed.

さらに、対物レンズ1と被測定物7との間に霧やちりな
どの粒子が浮遊していても、可視光よりも波長の長い赤
外単色光を使用しているために、透過率が大きく被測定
物7の発光ダイオード2からの光による照射は、極めて
効率よく行なわれる。
Furthermore, even if there are particles such as fog or dust floating between the objective lens 1 and the object to be measured 7, the transmittance is high because infrared monochromatic light with a longer wavelength than visible light is used. The object to be measured 7 is irradiated with light from the light emitting diode 2 very efficiently.

同様にして、対物レンズ1などに微小粒子が付着してい
ても、赤外単色光はこれらの粒子によって散乱すること
が少なく、空間フィルタ検出器4に達する光量が減少す
ることがない。
Similarly, even if microparticles adhere to the objective lens 1 or the like, infrared monochromatic light is rarely scattered by these particles, and the amount of light reaching the spatial filter detector 4 does not decrease.

なお、実施例では光源として赤外単色光を発する発光ダ
イオードを用いた場合を説明したが、本発明は実施例に
限定されるものでなく、光源として、外来光のスペクト
ル強度の弱い帯域に発光スペクトルを有する単色光でな
い赤外ランプを使用することも出来る。この場合には、
空間フィルタ検出器として赤外域に受光感度を有するG
eフォトダイオードを使用し、波長選択手段として赤外
透過フィルタを使用する。
In addition, in the example, a case was explained in which a light emitting diode that emits infrared monochromatic light was used as a light source, but the present invention is not limited to the example. Non-monochromatic infrared lamps with a spectrum can also be used. In this case,
G that has light receiving sensitivity in the infrared region as a spatial filter detector
An e-photodiode is used, and an infrared transmission filter is used as a wavelength selection means.

また、光源としてはこの他にも、半導体レーザを使用す
ることも出来る。
In addition to this, a semiconductor laser can also be used as the light source.

さらに、実施例では波長選択手段として干渉フィルタを
対物レンズの後段に配したものを説明したが、本発明は
実施例に限定されるものでなく、干渉フィルタを対物レ
ンズの前面に配することも出来る。このようにすると、
単色光が対物レンズを通過するので、対物レンズの色収
差の問題を解決することが出来て、空間フィルタ検出器
上に集束される光学像の鮮明度が向上し、検出信号のS
N比が向上する。
Further, in the embodiment, an interference filter is arranged after the objective lens as a wavelength selection means, but the present invention is not limited to the embodiment, and the interference filter may be arranged in front of the objective lens. I can do it. In this way,
Since the monochromatic light passes through the objective lens, it can solve the problem of chromatic aberration of the objective lens, improve the sharpness of the optical image focused on the spatial filter detector, and improve the S of the detection signal.
N ratio improves.

また、波長選択手段として空間フィルタ検出器自体に、
可視光帯域の受光感度を持たない波長選択特性を有する
ようにしてもよい。
In addition, the spatial filter detector itself is used as a wavelength selection means.
It may also have wavelength selection characteristics that do not have light receiving sensitivity in the visible light band.

[発明の効果] 本発明によれば、外来光の強度変動の影響を受けずに、
また外来光に基づく迷光の影響を受けずに、安定に精度
のよい速度検出を行なうことが出来る。また、被測定物
上に存在する異物質表面での反射光によってSN比が低
下することなく、常に高感度の速度検出が行なわれる。
[Effects of the Invention] According to the present invention, without being affected by intensity fluctuations of external light,
Furthermore, it is possible to stably and accurately detect speed without being affected by stray light caused by external light. In addition, high-sensitivity speed detection is always performed without reducing the signal-to-noise ratio due to light reflected from the surface of a foreign substance present on the object to be measured.

さらに、光源から照射光を長波長側に設定することによ
り、検出装置の開口部の汚れや検出装置と被測定物との
間に存在する霧やちりによる減衰がなく、常に高感度の
速度検出が行なわれる。
Furthermore, by setting the irradiation light from the light source to the long wavelength side, there is no attenuation due to dirt on the opening of the detection device or fog or dust that exists between the detection device and the measured object, and speed detection is always highly sensitive. will be carried out.

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

第1図は本発明の一実施例における空間フィル夕の説明
図、第2図は本発明の一実施例の動作を示す波長と放射
スペクトル強度及び透過率間の特性図、第3図は従来装
置の空間フィルタの説明図、第4図は従来装置の空間フ
ィルタ検出器の説明図、第5図及び第6図は従来装置で
の外来光の影響を示す説明図である。 1・・・・・・対物レンズ、2・・・・・・発光ダイオ
ード、3・・・・・・干渉フィルタ、4・・・・・・空
間フィルタ検出器、5・・・・・・プリアンプ、6・・
・・・・信号処理回路、7・・・・・・被謂定物。 第1図 第2図 シ皮 長 (、um) 第3図 / 第4図 第5図 第6図
Fig. 1 is an explanatory diagram of a spatial filter in an embodiment of the present invention, Fig. 2 is a characteristic diagram between wavelength, radiation spectrum intensity, and transmittance showing the operation of an embodiment of the present invention, and Fig. 3 is a conventional diagram. FIG. 4 is an explanatory diagram of the spatial filter of the device, FIG. 4 is an explanatory diagram of the spatial filter detector of the conventional device, and FIGS. 5 and 6 are explanatory diagrams showing the influence of extraneous light in the conventional device. 1...Objective lens, 2...Light emitting diode, 3...Interference filter, 4...Spatial filter detector, 5...Preamplifier , 6...
... Signal processing circuit, 7... Defined object. Figure 1 Figure 2 Skin length (,um) Figure 3 / Figure 4 Figure 5 Figure 6

Claims (1)

【特許請求の範囲】 1、被測定物を照射する光源と、前記被測定物の光学像
の移動方向に、所定のピッチで配列された複数個の受光
エレメントを備えた空間フィルタ検出器と、この空間フ
ィルタ検出器上に前記光学像を集束する結像光学系とで
空間フィルタが構成され、前記空間フィルタ検出器の光
電変換信号に基づいて、前記被測定物との相対速度を検
出する空間フィルタ式速度検出装置において、前記光源
として所定波長帯域の光を照射する光源が使用され、前
記空間フィルタに波長選択手段が設けられ、この波長選
択手段により前記空間フィルタ検出器に、前記光源の波
長帯域の光学像のみが集束されるように構成されてなる
ことを特徴とする空間フィルタ式速度検出装置。 2、請求項1の記載において、光源が赤外単色光光源で
あることを特徴とする空間フィルタ式速度検出装置。
[Scope of Claims] 1. A spatial filter detector including a light source that illuminates an object to be measured, and a plurality of light-receiving elements arranged at a predetermined pitch in the moving direction of an optical image of the object to be measured; A spatial filter is configured with an imaging optical system that focuses the optical image on the spatial filter detector, and a space that detects the relative velocity with the object to be measured based on the photoelectric conversion signal of the spatial filter detector. In the filter-type speed detection device, a light source that emits light in a predetermined wavelength band is used as the light source, and the spatial filter is provided with wavelength selection means, and the wavelength selection means causes the spatial filter detector to detect the wavelength of the light source. A spatial filter type speed detection device characterized in that it is configured so that only a band optical image is focused. 2. The spatial filter type speed detection device according to claim 1, wherein the light source is an infrared monochromatic light source.
JP8816388A 1988-04-12 1988-04-12 Space filter type speed detector Pending JPH01260366A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8816388A JPH01260366A (en) 1988-04-12 1988-04-12 Space filter type speed detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8816388A JPH01260366A (en) 1988-04-12 1988-04-12 Space filter type speed detector

Publications (1)

Publication Number Publication Date
JPH01260366A true JPH01260366A (en) 1989-10-17

Family

ID=13935259

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8816388A Pending JPH01260366A (en) 1988-04-12 1988-04-12 Space filter type speed detector

Country Status (1)

Country Link
JP (1) JPH01260366A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0430476U (en) * 1990-07-04 1992-03-11

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57172254A (en) * 1981-04-17 1982-10-23 Omron Tateisi Electronics Co Speed measuring device
JPS62191767A (en) * 1986-02-18 1987-08-22 Fujitsu Ten Ltd Space filter type ground speedometer

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57172254A (en) * 1981-04-17 1982-10-23 Omron Tateisi Electronics Co Speed measuring device
JPS62191767A (en) * 1986-02-18 1987-08-22 Fujitsu Ten Ltd Space filter type ground speedometer

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0430476U (en) * 1990-07-04 1992-03-11

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