JPS5910583Y2 - Photoconductor driving device - Google Patents

Photoconductor driving device

Info

Publication number
JPS5910583Y2
JPS5910583Y2 JP10161376U JP10161376U JPS5910583Y2 JP S5910583 Y2 JPS5910583 Y2 JP S5910583Y2 JP 10161376 U JP10161376 U JP 10161376U JP 10161376 U JP10161376 U JP 10161376U JP S5910583 Y2 JPS5910583 Y2 JP S5910583Y2
Authority
JP
Japan
Prior art keywords
voltage
photoconductor
intermittent
cds
capacitor
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
Application number
JP10161376U
Other languages
Japanese (ja)
Other versions
JPS5319268U (en
Inventor
正人 万井
浅治郎 荒井
Original Assignee
株式会社島津製作所
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 株式会社島津製作所 filed Critical 株式会社島津製作所
Priority to JP10161376U priority Critical patent/JPS5910583Y2/en
Publication of JPS5319268U publication Critical patent/JPS5319268U/ja
Application granted granted Critical
Publication of JPS5910583Y2 publication Critical patent/JPS5910583Y2/en
Expired legal-status Critical Current

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Classifications

    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy

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  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)

Description

【考案の詳細な説明】 この考案は光導電体駆動装置、特に光導電体を駆動する
ための付勢電源回路に関するものである。
DETAILED DESCRIPTION OF THE INVENTION This invention relates to a photoconductor driving device, and particularly to an energizing power supply circuit for driving a photoconductor.

CdS等の光導電体は光電管、フオ}}ランジスタ等の
受光素子にくらべて小形・軽量で高感度なので微細変調
光入力信号の検出に広く応用されている。
Photoconductors such as CdS are smaller, lighter, and more sensitive than light-receiving elements such as phototubes and transistors, and are therefore widely applied to detect finely modulated optical input signals.

CdS等の光導電体は一定の直流電圧を印加することに
より駆動され、その印加電圧の大きさに比例して一定の
人力光信号に対する出力が大きくなる。
A photoconductor such as CdS is driven by applying a constant DC voltage, and the output for a constant human optical signal increases in proportion to the magnitude of the applied voltage.

したがって微細変調光入力信号の検出感度を向上するに
は、光導電体を付勢する直流電圧を大きくすればよいこ
とになるが、直流電圧を大きくすると必然的に電源回路
が大きくなる。
Therefore, in order to improve the detection sensitivity of the finely modulated optical input signal, it is sufficient to increase the DC voltage that energizes the photoconductor, but increasing the DC voltage inevitably increases the size of the power supply circuit.

CdS等の光導電体を受光素子とする光検出装置は、例
えば血圧測定装置における血流信号または脈拍信号の検
出器等に適用されるので小形・軽量である必要があり、
駆動用直流電源としては電池が使用されている。
A photodetection device using a photoconductor such as CdS as a light receiving element is applied to, for example, a blood flow signal or pulse signal detector in a blood pressure measuring device, so it needs to be small and lightweight.
A battery is used as a driving DC power source.

一方光導電体を受光素子とする光検出装置は上記の血流
信号等の検出の場合、血管壁よりの血流で変調された微
細変調光信号を検出するので高感度である必要があると
共に長期間安定に動作するためには消費電力が少ないこ
とが要望されている。
On the other hand, when detecting the above-mentioned blood flow signals, a photodetector using a photoconductor as a light-receiving element detects finely modulated light signals modulated by blood flow from the blood vessel wall, so it needs to be highly sensitive and In order to operate stably for a long period of time, low power consumption is required.

この考案は上記に鑑み、電池等の小容量の直流電源でも
ってCdS等の光導電体を駆動する場合においても検出
感度が高く、消費電力の小さな駆動装置を提供しようと
するもので、CdS等の光導電体を直流電圧を間欠発振
器で間欠パルス電圧に変換し、この間欠パルス電圧を直
流化し、この直流化された電圧でもって駆動するように
したものである。
In view of the above, this idea aims to provide a drive device with high detection sensitivity and low power consumption even when driving a photoconductor such as CdS with a small-capacity DC power source such as a battery. The photoconductor is driven by converting a DC voltage into an intermittent pulse voltage using an intermittent oscillator, converting the intermittent pulse voltage into a DC voltage, and driving the photoconductor with the DC voltage.

以下図面によりこの考案を説明する。This invention will be explained below with reference to the drawings.

図においてOは発振回路で、実施例ではトランジスタQ
・間欠発振トランスT・抵抗R1・コンテ゛ンサC1と
で周知のプロツキング発振器を構戊している。
In the figure, O is an oscillation circuit, and in the example, transistor Q
- An intermittent oscillation transformer T, a resistor R1, and a capacitor C1 constitute a well-known blocking oscillator.

Eは直流電源としての電池である。E is a battery as a DC power source.

この電池Eの直流電圧はプロツキング発振回路Oで間欠
パルス電圧に変換され、間欠発振トランスTで昇圧され
る。
The direct current voltage of the battery E is converted into an intermittent pulse voltage by a blocking oscillation circuit O, and boosted by an intermittent oscillation transformer T.

図中イはその出力電圧波形を示す。A in the figure shows the output voltage waveform.

この昇圧されたパルス電圧は、間欠発振トランスTの2
次側に接続された整流器D2・コンテ゛ンサC2で整流
平滑されて直流化され、この直流化された電圧は負荷抵
抗R2を介してCdS(P)に印加されている。
This boosted pulse voltage is applied to the intermittent oscillation transformer T.
The voltage is rectified and smoothed by a rectifier D2 and a capacitor C2 connected to the next side and converted into a direct current, and this converted voltage is applied to CdS(P) via a load resistor R2.

上記構或において、CdS(P)に光が入射するとその
光の強さに応じてCdSの導電度が変化し、出力点Xに
光信号を対応した出力電圧が得られる。
In the above structure, when light is incident on the CdS(P), the conductivity of the CdS changes depending on the intensity of the light, and an output voltage corresponding to the optical signal is obtained at the output point X.

この場合この考案ではCdS(p)はパルス電圧をD2
で整流し、C2で積分して直流化した電圧で駆動されて
いるので、電源インピーダンスが高く、光の入射により
出力点Xに生ずる出力電圧は、従来の電池等の低インピ
ーダンス直流電源で駆動する場合にくらべて、同一の光
入力信号に対して大きな出力電圧が得られることになる
In this case, in this design, CdS(p) changes the pulse voltage to D2
Since it is driven by a voltage that is rectified by C2, integrated by C2, and converted to DC, the power source impedance is high, and the output voltage generated at output point X due to the incidence of light can be driven by a low impedance DC power source such as a conventional battery. This means that a larger output voltage can be obtained for the same optical input signal than in the case where the optical input signal is the same.

すなわち、CdSを電池等の直流電源で駆動するもので
は電源インピーダンスが低いので、CdSに光が入射す
ると出力点Xの電圧は負荷抵抗(R2)・CdS両者の
抵抗比で定まる出力電圧であるのに対し、CdSを間欠
パルス電圧で駆動するこの考案のものは電源インピーダ
ンスが極めて高いので、出力点Xには、上記の抵抗比で
定まる電圧と、CdSの導電度の変化により、間欠パル
ス電圧の出力点Yの電圧が変動し、この変化電圧とが重
畳した電圧が発生するので、同一の光入力信号に対し、
大きな出力信号が得られる。
In other words, when the CdS is driven by a DC power source such as a battery, the source impedance is low, so when light enters the CdS, the voltage at the output point X is the output voltage determined by the resistance ratio of the load resistance (R2) and the CdS. On the other hand, this device that drives CdS with intermittent pulse voltage has extremely high power source impedance, so at output point The voltage at output point Y fluctuates, and a voltage that is superimposed with this changing voltage is generated, so for the same optical input signal,
A large output signal can be obtained.

下表は同一電圧をCdsに従来の電池等よりの直流電源
で印加した場合と、第1図の間欠パルスの直流化電圧を
印加した場合の同一人力光信号に対する出力点Xに生ず
る出力電圧の実測結果を示すものである。
The table below shows the output voltage generated at the output point This shows actual measurement results.

なお、入力光信号としては図中に示すようにパルス幅Q
.lsec、パルス周期Q.5secの変調光入力信号
を使用した。
Note that the input optical signal has a pulse width Q as shown in the figure.
.. lsec, pulse period Q. A 5 sec modulated optical input signal was used.

上記の測定結果で明らがなように同一の印加電圧ならび
に同一の光入力に対し、この考案のものが約2倍の出力
電圧、換言すれば約2倍の検出感度が得られることにな
る。
As is clear from the above measurement results, for the same applied voltage and the same optical input, this device provides approximately twice the output voltage, or in other words, approximately doubles the detection sensitivity. .

以上のようにこの考案は直流電圧を間欠パルス電圧に変
換し、この間欠パルス電圧を直流化してCdS等の光導
電体に印加し、それを駆動するようにしたので、電源イ
ンピーダンスが高く検出感度が従来の電池等の直流電圧
で駆動するものに比し、向上すると共にパルス駆動であ
るので消費電力が少ないので長期間安定に動作する光導
電体駆動装置が得られる。
As described above, this invention converts DC voltage into intermittent pulse voltage, and converts this intermittent pulse voltage into DC and applies it to a photoconductor such as CdS to drive it, so the power source impedance is high and the detection sensitivity is high. The photoconductor driving device is improved in comparison with a conventional device driven by direct current voltage such as a battery, and because it is pulse driven, power consumption is low, so a photoconductor driving device that operates stably for a long period of time can be obtained.

また、検出感度が向上するので、従来のように電池等の
直流電圧を印加し、同一検出感度を得ようとするものに
比し、電源回路が簡素化し、光検出装置の小形化が可能
となる。
In addition, since the detection sensitivity is improved, the power supply circuit can be simplified and the photodetection device can be made more compact compared to conventional methods that apply DC voltage from a battery or other source to obtain the same detection sensitivity. Become.

さらに実施例のように間欠発振回路で変換されたパルス
電圧を昇圧するようにすれば、電池等の小さな直流電源
でもって検出感度の高い光導電体駆動装置が得られる。
Furthermore, if the pulse voltage converted by the intermittent oscillation circuit is boosted as in the embodiment, a photoconductor driving device with high detection sensitivity can be obtained using a small DC power source such as a battery.

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

図面はこの考案の実施例を示す回路図である。 E:電池、O:間欠発振回路(ブロッキング発振器)、
D2:整流器、C2:平滑用コンデンサ、R2:負荷回
路、P:CdS(光導電体)。
The drawing is a circuit diagram showing an embodiment of this invention. E: battery, O: intermittent oscillation circuit (blocking oscillator),
D2: Rectifier, C2: Smoothing capacitor, R2: Load circuit, P: CdS (photoconductor).

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 直流電源と、前記直流電源の電圧を入力としてこれを間
欠パルス電圧に変換する間欠発振器と、前記間欠発振器
から出力されるパルス電圧を直流化するための、整流器
及びコンテ゛ンサからなる整流平滑回路と、前記整流平
滑回路のコンデンサに並列に接続されてある負荷抵抗と
光導電体との直列回路とからなり、前記コンデンサの両
端から得られる直流電圧を前記負荷抵抗を介して前記光
導電体に駆動電圧として印加せしめてなる光導電体駆動
装置。
a rectifying and smoothing circuit consisting of a DC power supply, an intermittent oscillator that inputs the voltage of the DC power supply and converts it into an intermittent pulse voltage, and a rectifier and a capacitor for converting the pulse voltage output from the intermittent oscillator into DC; It consists of a series circuit of a photoconductor and a load resistor connected in parallel to the capacitor of the rectifying and smoothing circuit, and a DC voltage obtained from both ends of the capacitor is applied to the photoconductor as a driving voltage through the load resistor. A photoconductor driving device configured to apply an electric current to a photoconductor.
JP10161376U 1976-07-28 1976-07-28 Photoconductor driving device Expired JPS5910583Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10161376U JPS5910583Y2 (en) 1976-07-28 1976-07-28 Photoconductor driving device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10161376U JPS5910583Y2 (en) 1976-07-28 1976-07-28 Photoconductor driving device

Publications (2)

Publication Number Publication Date
JPS5319268U JPS5319268U (en) 1978-02-18
JPS5910583Y2 true JPS5910583Y2 (en) 1984-04-03

Family

ID=28711838

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10161376U Expired JPS5910583Y2 (en) 1976-07-28 1976-07-28 Photoconductor driving device

Country Status (1)

Country Link
JP (1) JPS5910583Y2 (en)

Also Published As

Publication number Publication date
JPS5319268U (en) 1978-02-18

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