JPH0295223A - Overheating detector - Google Patents
Overheating detectorInfo
- Publication number
- JPH0295223A JPH0295223A JP24806488A JP24806488A JPH0295223A JP H0295223 A JPH0295223 A JP H0295223A JP 24806488 A JP24806488 A JP 24806488A JP 24806488 A JP24806488 A JP 24806488A JP H0295223 A JPH0295223 A JP H0295223A
- Authority
- JP
- Japan
- Prior art keywords
- ccd
- optical system
- sunlight
- influence
- sunshine
- 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
Links
- 238000013021 overheating Methods 0.000 title claims description 6
- 238000003384 imaging method Methods 0.000 claims description 6
- 238000003331 infrared imaging Methods 0.000 claims description 5
- 238000001514 detection method Methods 0.000 claims description 3
- 230000003287 optical effect Effects 0.000 abstract description 10
- 230000005855 radiation Effects 0.000 abstract description 9
- 238000001444 catalytic combustion detection Methods 0.000 abstract 6
- 238000001228 spectrum Methods 0.000 description 9
- 238000000034 method Methods 0.000 description 5
- 230000003595 spectral effect Effects 0.000 description 5
- 230000035945 sensitivity Effects 0.000 description 4
- 238000005259 measurement Methods 0.000 description 3
- 230000005540 biological transmission Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- ZXEYZECDXFPJRJ-UHFFFAOYSA-N $l^{3}-silane;platinum Chemical compound [SiH3].[Pt] ZXEYZECDXFPJRJ-UHFFFAOYSA-N 0.000 description 1
- 230000005457 Black-body radiation Effects 0.000 description 1
- 241000276457 Gadidae Species 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000000295 emission spectrum Methods 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 229910021339 platinum silicide Inorganic materials 0.000 description 1
Landscapes
- Radiation Pyrometers (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、赤外線撮像により物体の温度を遠隔測定する
術に関し、特に太陽光の影響を除去して温度測定を行い
被測定体の過熱を検出する過熱検出装置に関する。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a technique for remotely measuring the temperature of an object using infrared imaging, and in particular, a technique for measuring temperature while removing the influence of sunlight to prevent overheating of the object to be measured. The present invention relates to an overheat detection device for detecting overheating.
従来、この種の赤外線撮像においては大気の窓と言われ
る3〜5μm帯か8〜12μm帯のいずれかを用いてい
る。前者の3〜5μm帯では太陽光の影響が大きく、昼
間晴天時には無視できない誤差を生じる。現在8〜12
μm帯が主流となりつつある要因の一つでもある。Conventionally, in this type of infrared imaging, either the 3-5 μm band or the 8-12 μm band, which is called the atmospheric window, is used. In the former 3 to 5 μm band, the influence of sunlight is large, causing a non-negligible error during daytime clear weather. Currently 8-12
This is also one of the reasons why the μm band is becoming mainstream.
しかし近年IR(Infra Red)CCDとして
、3〜4μm帯に感度のあるTV並の解像度、フレーム
数を有する撮像デバイスが開発され、この波長域でのリ
アルタイム撮像が容易になりつつある。However, in recent years, an imaging device has been developed as an IR (Infra Red) CCD that is sensitive in the 3 to 4 μm band and has a resolution and frame number comparable to that of a TV, and real-time imaging in this wavelength range is becoming easier.
赤外線撮像による物体の温度測定、特に送配電機材の過
熱検出を目的とする場合、昼間の測定に限られる為、太
陽光の影響の低減が実用上非常に重要である。一方現在
実用化されつつあるPt1S i IRCCD (白金
・シリサイド型IRCCD)は、短波長側に強い感度を
有する事から、その影響を受けやすい。このため太陽光
を除去する為にできる限り短波長側を光学的にカットす
る事が必要となっているが、このような対策では信号光
自体も低下していまうし、太陽光の影響の完全な除去は
困難である。When measuring the temperature of an object using infrared imaging, especially for detecting overheating of power transmission and distribution equipment, the measurement is limited to daytime, so reducing the influence of sunlight is of great practical importance. On the other hand, Pt1S i IRCCDs (platinum-silicide type IRCCDs), which are currently being put into practical use, have strong sensitivity on the short wavelength side and are therefore susceptible to this effect. For this reason, it is necessary to optically cut off the short wavelength side as much as possible in order to remove sunlight, but such measures also reduce the signal light itself and completely eliminate the influence of sunlight. Removal is difficult.
本発明によれば、2個のIRCCDを用い、2つの異な
る波長域の撮像を行い、太陽光の除去を実現する手段を
提供するものである。つまり、太陽光2信号光の放射ス
ペクトルを仮定して、2つの波長域のIRCCDからの
撮像結果より、太陽光の強度を推定して、それを除去す
るものである。According to the present invention, two IRCCDs are used to capture images in two different wavelength ranges, thereby providing means for realizing sunlight removal. That is, the intensity of sunlight is estimated and removed based on the imaging results from the IRCCD in two wavelength ranges, assuming the radiation spectrum of two signal lights of sunlight.
次に、本発明の一実施例を第1図にもとすいて説明する
。Next, one embodiment of the present invention will be described with reference to FIG.
第1図で1は被測定体、2は太陽光、3は赤外線撮像装
置の集光光学系、4は2つの波長域に光束を分割する光
学系で4− aグイクロイックミラー、4−bバンドパ
スフィルターより成る。5゜6は2つ17)IRCCD
、7はCCD駆動回路、8は増幅器、9は利得調整増幅
器、10は差動増幅器である。In Fig. 1, 1 is the object to be measured, 2 is the sunlight, 3 is the condensing optical system of the infrared imaging device, 4 is the optical system that splits the luminous flux into two wavelength ranges, 4-a gicchroic mirror, 4- It consists of a b-band pass filter. 5゜6 is two 17) IRCCD
, 7 is a CCD driving circuit, 8 is an amplifier, 9 is a gain adjustment amplifier, and 10 is a differential amplifier.
撮像デバイスであるIRCCDは第2図(a)に示す分
光感度特性を有する。一方太陽光のスペクトルは、59
00 Kの黒体放射に大気の透過特性を加えた形で表わ
せるが、代表的なスペクトル例を第2図(b)に実線で
示す。第2図(b)には同時に破線で常温物体の放射ス
ペクトルを示す。The IRCCD, which is an imaging device, has the spectral sensitivity characteristics shown in FIG. 2(a). On the other hand, the spectrum of sunlight is 59
It can be expressed by adding the atmospheric transmission characteristics to the blackbody radiation at 00 K, and a typical example of the spectrum is shown by the solid line in FIG. 2(b). At the same time, the dashed line in FIG. 2(b) shows the radiation spectrum of a room-temperature object.
被測定体1からの放射は、3の集光光学系で集光され、
IRCCD上に結像される。その放射は、被測定体自身
の温度による熱放射と、太陽光の反射より成る。4の波
長分割光学系で第2図(c)の破線を第1のCCD5の
利用波長域、実線を第2のCCD6の利用波長域とする
ように分割したとする。Radiation from the object to be measured 1 is focused by a focusing optical system 3,
The image is formed on the IRCCD. The radiation consists of thermal radiation due to the temperature of the object itself and reflection of sunlight. It is assumed that the wavelength division optical system of FIG. 2 (c) is divided so that the broken line in FIG.
単純化して第1のCODの利用波長をλ2〜λ2、第2
のCODの利用波長をλ1〜λ2とする。第1、第2の
CODの出力信号をそれぞれV、、V2とすれば
あるが、
と表わせる。ただし
R1はIRC,CDの分光感度特性(V/W、 p m
)Bλは太陽光スペクトル(W/μm)
S、は熱放射スペクトル(W/μm)
である。ここで第2図の(a)がRλ、(b)の実線が
Bλ、(b)の破線がSAに相当している。ここでより
求められる。ここで太陽光の除去を誤差少なく実行する
ためには〆はできるだけ大きく、bはできるだけ小さい
方が望ましい。つまりa>b
・・・・・・(6)従って(6)式が中間波長
λ2の決定要求となる。To simplify, the wavelength used for the first COD is λ2~λ2, and the wavelength used for the second COD is
The wavelengths used for COD are assumed to be λ1 to λ2. If the output signals of the first and second CODs are respectively V and V2, it can be expressed as follows. However, R1 is the spectral sensitivity characteristic (V/W, p m
) Bλ is the sunlight spectrum (W/μm) S is the thermal radiation spectrum (W/μm). Here, (a) in FIG. 2 corresponds to Rλ, a solid line in (b) corresponds to Bλ, and a broken line in (b) corresponds to SA. More required here. Here, in order to remove sunlight with less error, it is desirable that 〆 be as large as possible and b as small as possible. That is, a>b
(6) Therefore, equation (6) becomes a determination requirement for the intermediate wavelength λ2.
当然(6)式のaを大きくするためにはλ2が長波長で
あるほどよく、bを小さくするためには逆に短波長であ
るほどよい。Naturally, in order to increase a in equation (6), the longer the wavelength of λ2 is, the better, and conversely, in order to decrease b, the shorter the wavelength, the better.
測定精度を上げる為、できる限りSN比の良い測定が必
要である。従がって(5)式の直接測定されめる。これ
は(5)式より
とする。In order to improve measurement accuracy, it is necessary to perform measurements with as good a signal-to-noise ratio as possible. Therefore, equation (5) can be directly measured. This is based on equation (5).
真の信号成分は(1)式の第2項に比例するはずでを最
大にする事と等価である。1例として、第2図に示した
スペクトルを用いると、最適なλ2は、32μmである
事が計算できる。The true signal component is equivalent to maximizing the value that should be proportional to the second term of equation (1). As an example, using the spectrum shown in FIG. 2, it can be calculated that the optimum λ2 is 32 μm.
つまり、太陽光の影響を除去した信号は、第1のCCD
5出力から(第2のCCD6出力×−)を差し引いたも
のから得られる。In other words, the signal from which the influence of sunlight has been removed is transmitted to the first CCD.
It is obtained by subtracting (second CCD 6 output x -) from 5 output.
以上説明したように本発明では従来の、1つのIRCC
Dを用い、極力短波長側を光学フィルターでカットする
方法での、太陽光の除去と、信号光の低下と言う相反す
る事項を適切に解決する技術を提供するものである。As explained above, in the present invention, one IRCC
The present invention provides a technique for appropriately solving the conflicting issues of removing sunlight and reducing signal light by cutting off the short wavelength side as much as possible using an optical filter.
なお、この方式では、第2のIRCCDの出力に一定の
比率を乗じるが、その比率の決定が重要である。この比
率は、スペクトルを仮定して計算より求められる。最も
被測定体に近いと考えられる表面状態を持つ、反射板を
用い、太陽に直射した場合と、太陽に直接光らない場合
での指示目盛より実験的に比率を微調整する事により、
実際のスペクトルの変動にも対応できるものと考えられ
る。Note that in this method, the output of the second IRCCD is multiplied by a certain ratio, and determining the ratio is important. This ratio is obtained by calculation assuming a spectrum. By using a reflector with a surface condition that is considered to be closest to that of the object to be measured, and by experimentally fine-tuning the ratio based on the indication scale when it is directly exposed to the sun and when it is not directly exposed to the sun,
It is considered that this method can also deal with actual spectral fluctuations.
以上説明したように、本発明によれば2つの工RCCD
を用い、2つの波長域で撮像する事に声
よって太陽光の影響を相当軽減して温度検印することが
可能となる。As explained above, according to the present invention, there are two
By using the , it is possible to significantly reduce the influence of sunlight and check the temperature by capturing images in two wavelength ranges.
第1図は本発明の一実施例を示す図である。
l・・・・・・被測定体、2・・・・・・太陽光、3・
・・・・・集光光学系、4・・・・・・分割光学系、5
・・・・・・第1のIRCCD、6・・・・・・第2の
IRCCD、7・・・・・・CCD駆動回路、8・・・
・・・増幅器、9・・・・・・利得調整増幅器、10・
・・・・・差動増幅器、
第2図は各部の分光特性を示す図であり(a)はIRC
GfDの分光高感度特性、(b)は放射スペクトル、(
C)は分割スペクトルを示す。
代理人 弁理士 内 原 晋FIG. 1 is a diagram showing an embodiment of the present invention. l...Object to be measured, 2...Sunlight, 3.
...Condensing optical system, 4...Dividing optical system, 5
...First IRCCD, 6... Second IRCCD, 7... CCD drive circuit, 8...
...Amplifier, 9...Gain adjustment amplifier, 10.
...Differential amplifier, Figure 2 shows the spectral characteristics of each part, and (a) shows the IRC.
Spectral high sensitivity characteristics of GfD, (b) emission spectrum, (
C) shows the split spectrum. Agent Patent Attorney Susumu Uchihara
Claims (1)
熱部分を検出する過熱検出装置において、利用波長の異
なる2つの撮像素子で同時に物体を撮像し、第1の撮像
素子からの赤外画像からその物体の温度パターンを求め
るに際し、第2の撮像素子からのより短波長側の赤外画
像結果に一定比率を乗じたものを第一の撮像素子からの
赤外画像より差し引いて、太陽光の影響を低減させる事
を特徴とする過熱検出装置。In an overheating detection device that measures the surface temperature of an object using infrared imaging and detects overheated parts, two imaging devices using different wavelengths are used to simultaneously image the object, and the infrared image from the first imaging device is used to detect the object. When determining the temperature pattern, the infrared image result from the second image sensor on the shorter wavelength side is multiplied by a certain ratio and subtracted from the infrared image from the first image sensor to eliminate the influence of sunlight. An overheat detection device characterized by reducing overheating.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63248064A JP2758612B2 (en) | 1988-09-30 | 1988-09-30 | Overheat detector |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63248064A JP2758612B2 (en) | 1988-09-30 | 1988-09-30 | Overheat detector |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH0295223A true JPH0295223A (en) | 1990-04-06 |
JP2758612B2 JP2758612B2 (en) | 1998-05-28 |
Family
ID=17172669
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP63248064A Expired - Lifetime JP2758612B2 (en) | 1988-09-30 | 1988-09-30 | Overheat detector |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2758612B2 (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008241563A (en) * | 2007-03-28 | 2008-10-09 | Mitsubishi Heavy Ind Ltd | Dual-wavelength infrared image processing apparatus |
CN113758595A (en) * | 2020-12-02 | 2021-12-07 | 长春理工大学 | Resistance-type temperature pulsation appearance with solar irradiation and atmospheric pressure temperature compensation function |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5821526A (en) * | 1981-07-31 | 1983-02-08 | Mitsubishi Electric Corp | Detecting device using infrared ray |
JPS6191531A (en) * | 1984-10-12 | 1986-05-09 | Matsushita Electric Ind Co Ltd | Infrared camera unit |
-
1988
- 1988-09-30 JP JP63248064A patent/JP2758612B2/en not_active Expired - Lifetime
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5821526A (en) * | 1981-07-31 | 1983-02-08 | Mitsubishi Electric Corp | Detecting device using infrared ray |
JPS6191531A (en) * | 1984-10-12 | 1986-05-09 | Matsushita Electric Ind Co Ltd | Infrared camera unit |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008241563A (en) * | 2007-03-28 | 2008-10-09 | Mitsubishi Heavy Ind Ltd | Dual-wavelength infrared image processing apparatus |
CN113758595A (en) * | 2020-12-02 | 2021-12-07 | 长春理工大学 | Resistance-type temperature pulsation appearance with solar irradiation and atmospheric pressure temperature compensation function |
Also Published As
Publication number | Publication date |
---|---|
JP2758612B2 (en) | 1998-05-28 |
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