JPS60119179A - Infrared-ray image pickup device - Google Patents

Infrared-ray image pickup device

Info

Publication number
JPS60119179A
JPS60119179A JP58226358A JP22635883A JPS60119179A JP S60119179 A JPS60119179 A JP S60119179A JP 58226358 A JP58226358 A JP 58226358A JP 22635883 A JP22635883 A JP 22635883A JP S60119179 A JPS60119179 A JP S60119179A
Authority
JP
Japan
Prior art keywords
output
disturbance light
infrared
temperature
circuit
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
JP58226358A
Other languages
Japanese (ja)
Inventor
Tsutomu Yamaguchi
勉 山口
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP58226358A priority Critical patent/JPS60119179A/en
Publication of JPS60119179A publication Critical patent/JPS60119179A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04NPICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N5/00Details of television systems
    • H04N5/30Transforming light or analogous information into electric information
    • H04N5/33Transforming infrared radiation

Landscapes

  • Engineering & Computer Science (AREA)
  • Multimedia (AREA)
  • Signal Processing (AREA)
  • Radiation Pyrometers (AREA)
  • Transforming Light Signals Into Electric Signals (AREA)

Abstract

PURPOSE:To display with high performance under a wide temperature condition by providing the titled device with a device storing and generating a signal corresponding to disturbance light due to a temperature in a specific device and a detector detecting the temperature in the device and subtracting a disturbance light component included in an output from an infrared-ray detector by using said devices. CONSTITUTION:When the temperature of a part generating disturbance light 7 is T1 deg., an output NT1 from a corrected storage generating circuit 10 for generating a signal NT1 corresponding to the disturbance light 7 is applied to a multiplier 13. The circuit 10 is constituted by a storage device, e.g. a programmable read-only memory (PROM), the stored contents are programed by measuring the characteristics of the device and the reading timing 15 is read out synchronously with the output of a signal processing circuit 4. A subtractor 14 subtracts the output of the multiplier 13 from the output of the circuit 4, so that a high performance infrared-ray image pickup device completely preventing a video output from influence due to the disturbance light 7 can be provided.

Description

【発明の詳細な説明】 〔発明の技術分野〕 この発明は赤外線撮像装置の改良に関するものである。[Detailed description of the invention] [Technical field of invention] This invention relates to improvements in infrared imaging devices.

〔従来技術〕[Prior art]

第1図は従来の赤外線撮像装置であり2図において被写
体から放射される赤外線は、入射光(1)として結像光
学系(2)に入p、その出力は信号光(5)となり、赤
外線検出器(3)により検出され信号処理回路(4)に
よりモニタテレビ等に表示する為のビデオ信号に変換さ
れる。1方この装置で検出する赤外線は、一般にあらゆ
る物体から放射される為1例えば図に示す様に結像光学
系(2)の収納ケース(6)等から放射される赤外線は
、外乱光(7)として赤外線検出器に入る為、赤外線撮
像装置の性能を劣化させる欠点があった。
Figure 1 shows a conventional infrared imaging device. In Figure 2, the infrared rays emitted from the subject enter the imaging optical system (2) as incident light (1), and the output becomes signal light (5), which is infrared rays. The signal is detected by a detector (3) and converted by a signal processing circuit (4) into a video signal for display on a monitor television or the like. On the other hand, the infrared rays detected by this device are generally emitted from all kinds of objects.1 For example, as shown in the figure, the infrared rays emitted from the storage case (6) of the imaging optical system (2), etc. ), which has the disadvantage of deteriorating the performance of infrared imaging devices.

尚上記外乱光(7)は9種々の対策を施しても2元金に
しゃ断出来ずに、赤外線検出器(3)に入射される赤外
森光であり、又使用される周囲の温度及び撮像装置自身
の発熱によって変化する為装置の性能を大きく劣化させ
る一因となっている。
Incidentally, the above disturbance light (7) is infrared light that cannot be cut off into binary light even if nine various measures are taken and is incident on the infrared detector (3), and also due to the ambient temperature and Since it changes due to the heat generated by the imaging device itself, it is one of the causes of a significant deterioration in the performance of the device.

〔発明の概要〕[Summary of the invention]

この発明はかかる欠点を改善する目的でなされたもので
あり、前記外乱光(7)は、装置内の温度によシその光
量が変化することに着目し、ある特定の装置内温度によ
る外乱光相当信号を記憶発生させる装置と装置内温度を
検出する検出器を設け。
The present invention has been made with the aim of improving such drawbacks, and focuses on the fact that the amount of the ambient light (7) changes depending on the temperature inside the device. Equipped with a device that stores and generates the corresponding signal and a detector that detects the temperature inside the device.

これらをもとに赤外線検出器の出力に含まれた外乱光成
分を減算する事により、広範囲の温度条件で、良好な性
能を発揮する赤外線撮像装置を提供するものである。
By subtracting the disturbance light component contained in the output of the infrared detector based on these, an infrared imaging device that exhibits good performance under a wide range of temperature conditions is provided.

〔発明の実施例〕[Embodiments of the invention]

第2図はこの発明の一実施例を示すものであり0)〜(
7)は第1図に示した従来の装置と全く同じものである
。ここで外乱光(力の性質をまず説明すると一般にある
謔度゛Tの時の外乱光(カによる赤外線検出器(3)の
出力、NTは次式で表わされる。
FIG. 2 shows an embodiment of the present invention.
7) is exactly the same as the conventional device shown in FIG. Here, to first explain the nature of the disturbance light (power), the output of the infrared detector (3) due to the disturbance light (power), NT, when the disturbance level is generally ゛T, is expressed by the following equation.

NT−σ・T−に1・K2・K3 ・・ (1)ここで
 σ、ステンアン・ボルツマン定数′Y:外乱元を放射
する位置の絶対温度に1:外乱光を放射する位置の赤外
線放射率 に2:(σ・T−に1)の中で赤外線検出器(3)によ
り受光される比率 Kl赤外線検出器(3)の検出効率 (1)式において、ある撮像装置が使用される環境等で
変化する項目は、Tおよびに6である。従って前記(1
1式は次式の像に簡略化して表わせる。
NT-σ・T- is 1・K2・K3... (1) where σ is Sten-Ann-Boltzmann constant 'Y: Absolute temperature at the position where the disturbance source is radiated 1: Infrared emissivity at the position where the disturbance light is radiated 2: Ratio of light received by the infrared detector (3) in (σ・T−1) Kl Detection efficiency of the infrared detector (3) In equation (1), the environment in which a certain imaging device is used, etc. The items that change are T and 6. Therefore, the above (1
Equation 1 can be simplified and expressed as the image of the following equation.

NT =KO−TN −(21 但し、KO=σ・K1・K2 ・・・ (3)TN :
 T −K3 ・・・ (4)更にTNは温度、Tが判
明すれば製作した装置の特性を測定する事により容易に
算出する事が出来るO そこで1本発明では外乱光(7)f発生する部分の温度
が71度(例えは293度即ち20℃)の時に外乱光(
7)により赤外線検出器(3)の出力に現れる外乱相当
信号:NTl 全発生させる為の補正記憶発生回路O1
を設けその出カニTN1 ′!i7乗算回路峙に加える
。この補正信号記憶発生回路a1は、記憶装置例えばp
ROM:プログラマブル+)−トオ7リーメモリで構成
され、その記憶内容は装置の特性を測定して、フログラ
ムされ、その続出しタイミングαつは信号処理回路(4
)の出力と同期して読み出せる様になっている。
NT = KO-TN - (21 However, KO = σ・K1・K2... (3) TN:
T −K3 ... (4) Furthermore, TN is the temperature, and once T is known, it can be easily calculated by measuring the characteristics of the manufactured device. Therefore, in the present invention, disturbance light (7) f is generated. When the temperature of the part is 71 degrees (for example, 293 degrees or 20 degrees Celsius), the disturbance light (
7), the disturbance equivalent signal appearing in the output of the infrared detector (3): NTl Correction memory generation circuit O1 for generating all NTl
Set up that crab TN1'! Add to the i7 multiplier circuit. This correction signal storage generation circuit a1 has a storage device such as p
ROM (Programmable+) - consists of a 7-way memory, the stored contents are programmed by measuring the characteristics of the device, and the successive output timing α is determined by the signal processing circuit (4
) can be read out in synchronization with the output.

1万Ql)は外乱光(力を発生する部分の温度T2を検
出する為の温度検出器であり、その出力は補正定数発生
回路も3に与えられる。この補正定数発生回路aりは 但し TNl : Tiの時の(4)式相当値TN2°
T2の時の(4)式相当値 なる定数:に4を発生する様に、装置の特定を測定して
フログラムされている記憶装置で構成されてお怜、その
出カニに4は乗算回路−に与えられる。
10,000Ql) is a temperature detector for detecting the temperature T2 of the part that generates disturbance light (force), and its output is also given to the correction constant generation circuit 3.However, this correction constant generation circuit a is TNl. : Value TN2° equivalent to equation (4) for Ti
It consists of a memory device that measures and programs the specific characteristics of the device so as to generate a constant 4, which is the value equivalent to equation (4) at T2, and 4 is a multiplier circuit for the output. given to.

従って、乗算回路03の出カニNTM は次式で表わさ
れる。
Therefore, the output NTM of the multiplication circuit 03 is expressed by the following equation.

即ち、り6)式は(1)式で説明した外乱光(7)によ
る、赤外線検出器(3)の出力をめた事になり、信号処
理回路(4)の出力から減算回路aaにおいて1乗算回
路Q3の出力を減算する4番により、ビテオ出力は外乱
光(7)による影響を全く受けない高性能な赤外線撮像
装置を提供出来る。
In other words, Equation 6) calculates the output of the infrared detector (3) due to the disturbance light (7) explained in Equation (1), and the subtraction circuit aa calculates 1 from the output of the signal processing circuit (4). By subtracting the output of the multiplier circuit Q3, a high-performance infrared imaging device can be provided in which the video output is completely unaffected by the disturbance light (7).

尚、前記の如く補正信号発生回路aI及び補正記憶発生
回路圓の内容は装置の特定測定結果によって、フロクラ
ムされている為、前記温度による外乱光以外に内部で発
生する全ての外乱光2例えばナルシサス等をも本発明に
よって除去出来る事は言う捷でもない。
As mentioned above, since the contents of the correction signal generation circuit aI and the correction memory generation circuit yen are fluctuated according to the specific measurement results of the device, all the disturbance light generated internally in addition to the disturbance light caused by the temperature 2, for example, Narcissus. It is a matter of fact that the present invention can also eliminate such problems.

〔発明の効果〕〔Effect of the invention〕

以上説明した辿り2本発明によれば第2図の01〜aつ
を設ける事により、1吏用される周囲の温度及び装置自
身の発熱等により全く影響を受けない高い性能赤外?f
M撮像装置を提供出来る効果がるる。
As explained above, according to the present invention, by providing the units 01 to a shown in FIG. f
This has the effect of being able to provide M imaging devices.

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

第1図は、従来の赤外腺撮1象装置を示すブPツク図、
第2図は、この発明の一実施例を示すブロック図である
。 図において(3)は赤外線検出器、(4)は信号処理回
路、(7)は外乱光、 Qlは補正信号記憶発生回路、
(1υは温度検出器、02は補正定数発生回路、a騰は
乗算回路、 (141は減算回路である。 尚1図中同一行号は同−筐たは相当部分を示す。 代理人大岩増雄
FIG. 1 is a block diagram showing a conventional infrared gland imaging device;
FIG. 2 is a block diagram showing one embodiment of the present invention. In the figure, (3) is an infrared detector, (4) is a signal processing circuit, (7) is disturbance light, Ql is a correction signal storage generation circuit,
(1υ is a temperature detector, 02 is a correction constant generation circuit, a rise is a multiplication circuit, (141 is a subtraction circuit. The same line number in Figure 1 indicates the same case or a corresponding part. Agent Masuo Oiwa

Claims (1)

【特許請求の範囲】[Claims] ある特定の状態における赤外線検出器の出力に含まれる
不正信号を記憶する補正信号記憶発生回路と、赤外線撮
像装置内の温度を検出する温度検出器と、この温度検出
器の出力tもとに前記補正信号記憶発生回路の出力を補
正する補正定数発生回路とを備えた赤外線撮像装置。
a correction signal storage generation circuit that stores an incorrect signal included in the output of the infrared detector in a certain specific state; a temperature detector that detects the temperature within the infrared imaging device; An infrared imaging device comprising a correction constant generation circuit that corrects the output of the correction signal storage generation circuit.
JP58226358A 1983-11-30 1983-11-30 Infrared-ray image pickup device Pending JPS60119179A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58226358A JPS60119179A (en) 1983-11-30 1983-11-30 Infrared-ray image pickup device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58226358A JPS60119179A (en) 1983-11-30 1983-11-30 Infrared-ray image pickup device

Publications (1)

Publication Number Publication Date
JPS60119179A true JPS60119179A (en) 1985-06-26

Family

ID=16843896

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58226358A Pending JPS60119179A (en) 1983-11-30 1983-11-30 Infrared-ray image pickup device

Country Status (1)

Country Link
JP (1) JPS60119179A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01110225A (en) * 1987-10-23 1989-04-26 Agency Of Ind Science & Technol Infrared radiation meter
US5448319A (en) * 1992-09-22 1995-09-05 Olympus Optical Co., Ltd. Optical system for monitor cameras to be mounted on vehicles
WO1997017887A1 (en) * 1995-11-13 1997-05-22 Citizen Watch Co., Ltd. Clinical radiation thermometer

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01110225A (en) * 1987-10-23 1989-04-26 Agency Of Ind Science & Technol Infrared radiation meter
US5448319A (en) * 1992-09-22 1995-09-05 Olympus Optical Co., Ltd. Optical system for monitor cameras to be mounted on vehicles
US5648835A (en) * 1992-09-22 1997-07-15 Olympus Optical Co., Ltd. Optical system for monitor cameras to be mounted on vehicles
WO1997017887A1 (en) * 1995-11-13 1997-05-22 Citizen Watch Co., Ltd. Clinical radiation thermometer
US6155712A (en) * 1995-11-13 2000-12-05 Citizen Watch Co., Ltd. Radiation clinical thermometer

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