JPS6116011B2 - - Google Patents
Info
- Publication number
- JPS6116011B2 JPS6116011B2 JP54051394A JP5139479A JPS6116011B2 JP S6116011 B2 JPS6116011 B2 JP S6116011B2 JP 54051394 A JP54051394 A JP 54051394A JP 5139479 A JP5139479 A JP 5139479A JP S6116011 B2 JPS6116011 B2 JP S6116011B2
- Authority
- JP
- Japan
- Prior art keywords
- detection element
- output
- signal
- electromagnetic waves
- synchronization signal
- 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
Links
Classifications
-
- 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
Landscapes
- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Radiation Pyrometers (AREA)
Description
【発明の詳細な説明】
本発明は放射温度計等、電磁波を計測媒体、若
しくは計測対象とする光学的測定装置に関するも
のである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical measurement device such as a radiation thermometer that uses electromagnetic waves as a measurement medium or measurement target.
この種、電磁波を計測媒体、若しくは計測対象
とする光学測定装置としては放射温度計の他にも
照度計、輝度計、透過率計等があり、その検出素
子としては一般に熱電堆、サーミスタ・ボロメー
タ等の熱電対形検出素子、若しくはSi,PbS,
PbSe等の光電形検出素子が用いられる。こうし
た検出素子は非線形の特性を有しているので計測
に都合の良い特性の範囲は限られており、それ
故、高精度の測定装置とするには狭い範囲内を計
測する測定装置にならざるを得なかつた。 In addition to radiation thermometers, this type of optical measurement device that uses electromagnetic waves as a measurement medium or measurement object includes illumination meters, luminance meters, transmittance meters, etc., and their detection elements are generally thermoplates, thermistors, and bolometers. Thermocouple type detection element such as Si, PbS,
A photoelectric detection element such as PbSe is used. Since these detection elements have nonlinear characteristics, the range of characteristics that are convenient for measurement is limited, and therefore, in order to be a highly accurate measuring device, it must be a measuring device that measures within a narrow range. I didn't get it.
本発明は以上のような点に鑑み、チヨツパとし
ての機能を有する回転盤の透過窓に互いに透過率
を異にする2個以上の減光フイルタ若しくは互い
に透過波長を異にする有色フイルタを挿着し、各
フイルタのなかで任意のフイルタを介して検出素
子に照射された電磁波による検出素子出力を選択
して、その電磁波のエネルギー量を出力信号とし
て出力する構成とすることにより、広い範囲に渡
つて精度の高い計測を行うことができる光学的測
定装置を提供することを目的とするものである。 In view of the above points, the present invention has been developed by inserting two or more neutral density filters having mutually different transmittances or colored filters having mutually different transmission wavelengths into the transmitting window of a rotary disk that functions as a chopper. However, by selecting the detection element output from the electromagnetic waves irradiated to the detection element through an arbitrary filter among each filter and outputting the energy amount of the electromagnetic waves as an output signal, it is possible to spread over a wide range. The object of the present invention is to provide an optical measuring device that can perform highly accurate measurements.
次に、本発明に係る装置を放射温度計に応用し
た際の第1の実施例を説明する。 Next, a first example in which the device according to the present invention is applied to a radiation thermometer will be described.
第1図は放射温度計の機構説明図であり、この
放射温度計1の前面には対物レンズ2が設けら
れ、該対物レンズ2の後方に回転盤3が設けられ
ている。この回転盤3はその中心がモータ4の回
転軸4aと接続されて一定速度で回転せしめられ
ており、更に、その回転中心から等距離位置に複
数個の透過窓5が形成されている。この実施例に
おいては上記透過窓5として4個の透過窓5a,
5b,5c,5dが形成されており、それぞれの
透過窓5a,5b,5c,5dには互いに透過率
を異にする減光フイルタ6a,6b,6c,6d
が挿着されている。更に、上記回転盤3の後方に
検出素子8が設けられており、この検出素子8に
は前記対物レンズ2と透過窓5のうちのひとつと
を結ぶ一直線上に位置せしめられている。この検
出素子8は熱電堆、サーミスタ・ポロメータ等の
熱電形検出素子、若しくはSi,PbS,PbSe等の光
電形検出素子が用いられており、該検出素子8の
出力は増幅器9に入力されている。 FIG. 1 is an explanatory view of the mechanism of a radiation thermometer. An objective lens 2 is provided on the front side of the radiation thermometer 1, and a rotary disk 3 is provided behind the objective lens 2. The rotary disk 3 has its center connected to the rotating shaft 4a of the motor 4 and is rotated at a constant speed, and furthermore, a plurality of transparent windows 5 are formed at positions equidistant from the rotation center. In this embodiment, the transmission windows 5 include four transmission windows 5a,
5b, 5c, and 5d are formed, and each transmission window 5a, 5b, 5c, and 5d is provided with a neutral density filter 6a, 6b, 6c, and 6d having different transmittances.
is inserted. Furthermore, a detection element 8 is provided behind the rotary disk 3, and the detection element 8 is positioned on a straight line connecting the objective lens 2 and one of the transmission windows 5. The detection element 8 is a thermoelectric detection element such as a thermopile, a thermistor/porometer, or a photoelectric detection element such as Si, PbS, PbSe, etc., and the output of the detection element 8 is input to an amplifier 9. .
また、上記回転円盤3の外周に近接して同期信
号発生器7が設けられおり、この同期信号発生器
7は上記透過窓5と対応する数、即ちこの実施例
においては4個の同期信号発生器7a,7b,7
c,7dが設けられ、この同期信号発生器として
近接スイツチ、光電管等が用いられている。この
各同期信号発生器7a,7b,7c,7dは透過
窓5a,5b,5c,5dの夫々と対応して、透
過窓5が対物レンズ2と検出素子8とを結ぶ一直
線上に位置した際にはそれぞれ対応する同期信号
発生器7a乃至7dより同期信号P1乃至P4が出力
せしめられるように構成されている。上記同期信
号発生器7は切換スイツチ10を介して信号分離
回路11に接続され、同期信号Pが該回路11に
入力されると共に、この信号分離回路11には前
記増幅器9からの出力信号eが入力されている。 Further, a synchronizing signal generator 7 is provided close to the outer periphery of the rotating disk 3, and this synchronizing signal generator 7 has a number corresponding to the number of transmitting windows 5, that is, four synchronizing signal generators in this embodiment. Vessels 7a, 7b, 7
A proximity switch, a phototube, etc. are used as synchronizing signal generators. These synchronizing signal generators 7a, 7b, 7c, and 7d correspond to the transmission windows 5a, 5b, 5c, and 5d, respectively, when the transmission window 5 is located on a straight line connecting the objective lens 2 and the detection element 8. are configured such that synchronizing signals P1 to P4 are outputted from corresponding synchronizing signal generators 7a to 7d, respectively. The synchronization signal generator 7 is connected to a signal separation circuit 11 via a changeover switch 10, and the synchronization signal P is input to the circuit 11, and the signal separation circuit 11 receives the output signal e from the amplifier 9. It has been entered.
更にこの信号分離回路11は整流回路12に接
続されており、上記同期信号Pが加えられた際に
導通状態となり出力信号eを整流回路12に加え
る構成、即ちスイツチング回路とされている。上
記整流回路12は上記回転円盤3により直流―交
流変換された信号をふたたび直流信号に変換する
構成とされ、この整流回路12により出力される
温度計出力aは記録計器、自動制御等に供給され
ている。 Furthermore, this signal separation circuit 11 is connected to a rectifier circuit 12, and when the synchronizing signal P is applied, it becomes conductive and applies an output signal e to the rectifier circuit 12, that is, it is a switching circuit. The rectifier circuit 12 is configured to convert the signal converted from DC to AC by the rotating disk 3 into a DC signal again, and the thermometer output a outputted by the rectifier circuit 12 is supplied to a recording instrument, automatic control, etc. ing.
以上の構成による放射温度計1の作用を以下に
説明する。 The operation of the radiation thermometer 1 with the above configuration will be explained below.
被測定体よりの放射エネルギーが対物レンズ2
を介して回転盤3に照射されると、この放射エネ
ルギーは回転盤3が常に回転状態とされているこ
とから間欠的に透過窓5を通過して断続的に検出
素子8に照射される。即ち上記回転盤3はチヨツ
パとしての機能を有し、直流―交流変換を行つて
いると共に、その透過窓5a乃至5dには夫々互
いに透過率の異なる減光フイルタ6a乃至6dが
挿着されていることから次々と減衰された放射エ
ネルギーが検出素子8に照射されることになり、
この検出素子8から増幅器9を介して出力される
出力信号eとして第2図に示すように出力信号e1
乃至e4が繰り返し現れることになる。この出力信
号eは信号分離回路11において、同期信号発生
器7からの同期信号Pにより選択されて、所望の
出力信号e1〜4が整流回路12でふたたび直流信
号に変換され、この温度計の出力aとして出力さ
れる。更に詳細には上記同期信号Pは同期信号発
生器7a乃至7dと、それぞれ対応する透過窓5
a乃至5dが対物レンズ2と検出素子8とを結ぶ
一直線上に位置した際に発生され、例えば一番大
きな透過率を有する透過窓5aが対物レンズ2と
検出素子8とを結ぶ一直線上に位置した際には同
期信号発生器7aが同期信号P1を発生する。この
とき切換スイツチ10が同期信号発生器7aを選
択している場合には信号分離回路11に同期信号
P1が加えられ、この同期信号P1は切換スイツチ1
0を他に切り換えるまで繰返される。この同期信
号P1は検出素子8からの出力信号eのなかで透過
窓5aを通過した放射エネルギーによる出力信号
e1と時間的に一致せしめられているので、整流回
路12を介して出力される温度計出力aとして出
力信号e1が整流されてなる直流信号a1が出力され
る。 The radiation energy from the object to be measured is transmitted to the objective lens 2.
When the rotary disk 3 is irradiated with the radiant energy, since the rotary disk 3 is always in a rotating state, this radiant energy passes through the transmission window 5 intermittently and is intermittently irradiated onto the detection element 8. That is, the rotary disk 3 has a function as a chopper and performs DC-AC conversion, and at the same time, dark filters 6a to 6d having different transmittances are inserted into the transmission windows 5a to 5d, respectively. Therefore, the detection element 8 is irradiated with radiant energy that is attenuated one after another.
As the output signal e outputted from the detection element 8 via the amplifier 9, the output signal e 1 is as shown in FIG.
to e 4 will appear repeatedly. This output signal e is selected in the signal separation circuit 11 by the synchronization signal P from the synchronization signal generator 7, and the desired output signals e1 to e4 are converted into a DC signal again in the rectification circuit 12, and the thermometer is It is output as output a. More specifically, the synchronization signal P is transmitted to the synchronization signal generators 7a to 7d and the corresponding transmission windows 5.
It is generated when windows a to 5d are located on a straight line connecting the objective lens 2 and the detection element 8. For example, the transmission window 5a having the largest transmittance is located on the straight line connecting the objective lens 2 and the detection element 8. When this occurs, the synchronization signal generator 7a generates the synchronization signal P1 . At this time, if the changeover switch 10 selects the synchronization signal generator 7a, the synchronization signal is sent to the signal separation circuit 11.
P 1 is applied, and this synchronizing signal P 1 is applied to changeover switch 1.
This will be repeated until you switch 0 to something else. This synchronization signal P1 is an output signal due to the radiant energy that has passed through the transmission window 5a in the output signal e from the detection element 8.
Since the time is made to coincide with e 1 , the DC signal a 1 obtained by rectifying the output signal e 1 is output as the thermometer output a outputted via the rectifier circuit 12 .
また切換スイツチ10が他の同期信号発生器7
b乃至7dに切り換えられた際には同様に夫々対
応する出力信号e2乃至e4のいずれかが温度計出力
aとして出力されることになる。こうして出力さ
れる温度計出力a1乃至a4は第3図に示すように
夫々の温度範囲において適当な特性を有してお
り、例えば第4図に示すような表示装置16を用
いることにより温度を知ることができる。この表
示装置16には温度計出力a1乃至a4と対応する目
盛17a,17b,17c,17dが記載されて
おり、それぞれの目盛17は上記温度計出力a1乃
至a4の非線形特性に合わせて不等間隔で刻まれて
いる。 Also, the changeover switch 10 is connected to another synchronous signal generator 7.
When the switches are switched to b to 7d, one of the corresponding output signals e 2 to e 4 is similarly output as the thermometer output a. The thermometer outputs a 1 to a 4 outputted in this way have appropriate characteristics in each temperature range as shown in FIG. can be known. This display device 16 has scales 17a, 17b, 17c, and 17d corresponding to the thermometer outputs a1 to a4 , and each scale 17 is set in accordance with the nonlinear characteristics of the thermometer outputs a1 to a4 . carved at uneven intervals.
次に、本発明に係る装置を放射温度計に応用し
た第2乃至第4の実施例を第5乃至7図について
説明する。 Next, second to fourth embodiments in which the device according to the present invention is applied to a radiation thermometer will be described with reference to FIGS. 5 to 7.
尚、上述した第1の実施例と同等の箇所には同
様の符号を付しその説明を省略する。 Note that the same reference numerals are given to the same parts as in the first embodiment described above, and the explanation thereof will be omitted.
第5図は同期発生装置7を一個だけ用いると共
に、パルスシフト回路13を用いた場合の第2の
実施例を示すものであり、この同期発生装置7は
全部の透過窓5a乃至5dの位置を検出する構成
とされ、その同期信号Pはパルスシフト回路13
に入力されている。このパルスシフト回路13は
透過窓5と同数の出力端子13a乃至13dを有
しており、この出力端子13a乃至13dには順
番に上記同期信号Pが繰り返し加えられる構成と
されている。 FIG. 5 shows a second embodiment in which only one synchronization generator 7 is used and a pulse shift circuit 13 is used. The synchronizing signal P is detected by the pulse shift circuit 13.
has been entered. This pulse shift circuit 13 has the same number of output terminals 13a to 13d as the transmission windows 5, and is configured to repeatedly apply the synchronizing signal P to the output terminals 13a to 13d in order.
然して、切換スイツチ10が選択している出力
端子13a乃至13dに応じて信号分離回路11
における出力信号e1乃至e4のいずれかが選択され
ることになる。 Therefore, the signal separation circuit 11 is selected depending on the output terminals 13a to 13d selected by the changeover switch 10.
One of the output signals e 1 to e 4 is selected.
第6図は透過窓5の数と同数の信号分離回路1
1を用いた場合の第3の実施例を示すものであ
り、同期信号発生装置7a乃至7dからの同期信
号P1乃至P4はそれぞれ専用の信号分離回路11a
乃至11dに入力されており、増幅器9からの出
力信号eは上記全部の信号分離回路11a乃至1
1dに加えられている。更に、この各信号分離回
路11a乃至11dは切換スイツチ10を介して
整流回路12に接続されている。 Figure 6 shows the same number of signal separation circuits 1 as the number of transmission windows 5.
1 is used, and the synchronization signals P 1 to P 4 from the synchronization signal generators 7 a to 7 d are sent to dedicated signal separation circuits 11 a, respectively.
The output signal e from the amplifier 9 is input to all the signal separation circuits 11a to 11d.
It has been added to 1d. Further, each of the signal separation circuits 11a to 11d is connected to a rectifier circuit 12 via a changeover switch 10.
第7図は前述した第1の実施例による放射温度
計にレンジ自動切換装置を付加した場合の第4の
実施例を示すものであり、レンジ自動切換装置と
してコンパレータ14が用いられている。このコ
ンパレータ14は基準設定器15と整流器12か
らの出力値を入力としており、整流器12からの
出力値が上限所定値を越えた際と下限の所定値を
下回つた際に出力する構成とされ、このコンパレ
ータ14の出力により切換スイツチ10が順次切
換えられて適正な出力信号eが自動的に選択され
ている。 FIG. 7 shows a fourth embodiment in which an automatic range switching device is added to the radiation thermometer according to the first embodiment, and a comparator 14 is used as the automatic range switching device. This comparator 14 receives the output values from the reference setter 15 and the rectifier 12 as input, and is configured to output when the output value from the rectifier 12 exceeds a predetermined upper limit value and falls below a predetermined lower limit value. , the selector switch 10 is sequentially switched by the output of the comparator 14, and the appropriate output signal e is automatically selected.
尚、上述の各実施例では減光フイルタが用いら
れているが互いに透過波長を異にする有色フイル
タを用いる構成としても良い。 Incidentally, although a neutral density filter is used in each of the above-mentioned embodiments, a configuration may also be adopted in which colored filters having mutually different transmission wavelengths are used.
以上説明したように本発明によればチヨツパと
しての機能を有する回転盤の透過窓に互いに透過
率を異にする2個以上の減光フイルタ若しくは互
いに透過波長を異にする有色フイルタを挿着し、
各フイルタのなかで任意のフイルタを介して検出
素子に照射された電磁波による検出素子出力を選
択して、その電磁波のエネルギー量を出力信号と
して出力する構成としたので、広い範囲に渡つて
精度の高い計測を行うことができる光学的測定装
置を提供することができる効果がある。 As explained above, according to the present invention, two or more neutral density filters having mutually different transmittances or colored filters having mutually different transmittance wavelengths are inserted into the transmitting window of the rotary disk which functions as a chopper. ,
The configuration is such that the detection element output from the electromagnetic waves irradiated to the detection element through an arbitrary filter is selected from each filter, and the energy amount of the electromagnetic waves is output as an output signal, so accuracy can be improved over a wide range. This has the effect of providing an optical measuring device that can perform high-quality measurements.
第1図は本発明に係る装置を放射温度計に応用
した際の第1の実施例を示す機構説明図、第2図
は出力信号eと同期信号Pとの関係を示すグラフ
図、第3図は温度計出力と温度との関係を示すグ
ラフ図、第4図は表示装置の正面図、第5・6・
7図は第2・3・4の実施例を示す機構説明図で
ある。
3…回転盤、5…透過窓、6…フイルタ、7…
同期信号発生装置、8…検出素子、11…信号分
離回路。
FIG. 1 is a mechanism explanatory diagram showing a first embodiment in which the device according to the present invention is applied to a radiation thermometer, FIG. 2 is a graph diagram showing the relationship between the output signal e and the synchronization signal P, and FIG. The figure is a graph showing the relationship between thermometer output and temperature, Figure 4 is a front view of the display device, and Figures 5, 6, and
FIG. 7 is a mechanism explanatory diagram showing the second, third, and fourth embodiments. 3...Rotary disk, 5...Transmission window, 6...Filter, 7...
Synchronous signal generator, 8...detection element, 11...signal separation circuit.
Claims (1)
ての電磁波を検出する検出素子と、この検出素子
までの電磁波の伝搬経路の途中に設けられる2個
以上の透過窓を有する回転盤と、上記透過窓に挿
着されるフイルタと、その透過窓の位置を検出す
る同期信号発生装置と、該同期信号発生装置の同
期信号により上記検出素子からの検出信号を選択
分離せしめる信号分離回路とを具備しており、上
記フイルタは互いに透過率を異にする減光フイル
タ若しくは互いに透過波長を異にする有色フイル
タとされ、上記各フイルタのなかで任意のフイル
タを介して検出素子に照射された電磁波による検
出素子出力を選択してその電磁波のエネルギー量
を出力信号として出力する構成とされたことを特
徴とする光学的測定装置。1. At least a detection element for detecting electromagnetic waves as a measurement medium or measurement target, a rotary disk having two or more transmission windows provided in the middle of the propagation path of the electromagnetic waves to the detection element, and a rotary disk that is inserted into the transmission windows. the filter, a synchronization signal generation device for detecting the position of the transmission window, and a signal separation circuit for selectively separating the detection signal from the detection element using the synchronization signal of the synchronization signal generation device; The filters are neutral density filters with mutually different transmittances or colored filters with mutually different transmission wavelengths, and the detection element output is selected based on the electromagnetic waves irradiated to the detection element through any one of the above filters. An optical measuring device characterized in that it is configured to output the energy amount of the electromagnetic waves as an output signal.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5139479A JPS55143418A (en) | 1979-04-27 | 1979-04-27 | Optical measuring instrument |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5139479A JPS55143418A (en) | 1979-04-27 | 1979-04-27 | Optical measuring instrument |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS55143418A JPS55143418A (en) | 1980-11-08 |
| JPS6116011B2 true JPS6116011B2 (en) | 1986-04-26 |
Family
ID=12885712
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5139479A Granted JPS55143418A (en) | 1979-04-27 | 1979-04-27 | Optical measuring instrument |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS55143418A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5952661A (en) * | 1996-08-16 | 1999-09-14 | Raytheon Company | Chopper for thermal imaging system and method |
-
1979
- 1979-04-27 JP JP5139479A patent/JPS55143418A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS55143418A (en) | 1980-11-08 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US3611805A (en) | Radiation thermometer | |
| US3057200A (en) | Pyrometer | |
| US4389118A (en) | Color meter | |
| US2674155A (en) | Pyrometer | |
| US2658390A (en) | Radiation pyrometry | |
| JPS6116011B2 (en) | ||
| US2488430A (en) | Method and apparatus for measuring the dimensions of objects by the radiation differential between the object to be measured and a comparison object | |
| JPS58139037A (en) | 2-color thermometer | |
| US3222930A (en) | Spectropyrometer apparatus and method | |
| JPS6283625A (en) | optical power meter | |
| JPS6111368B2 (en) | ||
| US3653772A (en) | Two lamp light comparison type densitometer | |
| US3376748A (en) | Method and apparatus for radiation pyrometry | |
| US2759392A (en) | Color temperature meter and color analyzer | |
| JPS5910485B2 (en) | 2 channel photometry device | |
| JPS6355426A (en) | Radiation thermometer | |
| JPH05264352A (en) | Spectrophotometer | |
| JPS6029705Y2 (en) | Radiation temperature measurement device | |
| US4119988A (en) | Camera using instant print film | |
| JP2551177B2 (en) | Measuring device | |
| SU746207A1 (en) | Method and apparatus for remote temperature measuring | |
| JPS58166226A (en) | Photoelectric transducer | |
| SU709958A1 (en) | Spectral ratio pyrometer | |
| JPH04355308A (en) | Multilayer film thickness measuring device | |
| JPH04353727A (en) | Two-color radiation thermometer |