JPS592080B2 - Nisenshikisitsudohatsushinki - Google Patents
NisenshikisitsudohatsushinkiInfo
- Publication number
- JPS592080B2 JPS592080B2 JP50116934A JP11693475A JPS592080B2 JP S592080 B2 JPS592080 B2 JP S592080B2 JP 50116934 A JP50116934 A JP 50116934A JP 11693475 A JP11693475 A JP 11693475A JP S592080 B2 JPS592080 B2 JP S592080B2
- Authority
- JP
- Japan
- Prior art keywords
- temperature
- humidity
- master station
- resistance
- voltage
- 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
Landscapes
- Investigating Or Analyzing Materials By The Use Of Fluid Adsorption Or Reactions (AREA)
- Dc Digital Transmission (AREA)
- Arrangements For Transmission Of Measured Signals (AREA)
- Indication And Recording Devices For Special Purposes And Tariff Metering Devices (AREA)
Description
【発明の詳細な説明】
本発明は子局における湿度の状態を親局に発信する様に
した二線式湿度発信器に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a two-wire humidity transmitter that transmits the humidity status at a slave station to a master station.
本発明の目的は子局における湿度検出を子局に温度雰囲
気の影響を補償する様に構成して親局に発信する様にし
た二線式湿度発信器に係る。An object of the present invention is to provide a two-wire humidity transmitter in which humidity detection in a slave station is configured to compensate for the influence of temperature atmosphere on the slave station and transmitted to a master station.
相対湿度は温度に依存し、例えば第5図に示す様に温度
によつて異る値を示す。従来に於ては五線式或は四線式
の伝送線を使用し、子局における湿度及び温度を測定し
五線式では一本をコンモンとし、四線式では二本づつの
対によつて親局に信号伝送している。しかし、子局が多
数あり、しかもビルデング等に於て建築の際に設けた配
管に他の信号線と共に内挿する場合に於ては、伝送線の
数が多い事は経済的でないばかりか、手数を要するもの
である事は云うまでもない。本発明は二線の伝送線によ
つて、子局における湿度及び温度の状態を同時に親局に
伝送し、且つ電源は、それぞれの子局に設ける事なく、
親局にのみ設け、親局より子局に対し電気勢力を与え、
子局における状態の変化に応じて生じる該電気勢力の変
化量を再び親局に於て取出し且つ演算する事によつて、
相対湿度の温度に依存しない真なる相対湿度値を得る様
に構成したものである。Relative humidity depends on temperature, and exhibits different values depending on temperature, as shown in FIG. 5, for example. Conventionally, a five-wire or four-wire transmission line is used to measure humidity and temperature at a slave station. and transmits signals to the master station. However, when there are a large number of slave stations and the signal line is interpolated along with other signal lines into piping installed during construction, it is not only uneconomical to have a large number of transmission lines. Needless to say, it is time-consuming. The present invention simultaneously transmits the humidity and temperature conditions at the slave station to the master station using two transmission lines, and without providing a power supply to each slave station.
It is installed only in the master station, and gives electric power to the slave stations from the master station.
By retrieving and calculating at the master station the amount of change in the electrical force that occurs in response to changes in the state at the slave station,
It is configured to obtain a true relative humidity value that is independent of relative humidity temperature.
第1図に於て、親局10は中央監視部に設けてあり、二
本の伝送線rl、に2によつて子局20に連結してある
。親局10に於て、スイッチ51、52は定電圧電源E
の電気勢力を子局20に交互に逆方向に与える様にフリ
ップフロップ回路等で切換えるもので、それぞれ等しい
時間毎に共通端子Cl、C2から端子al、a2側及び
bl、b2側に切換えるものである。Rsは取出端子1
1、12間に接続された基準抵抗である。子局20に於
て、電気抵抗式湿度検出器等の湿度一抵抗値変化体Rh
とサーミスタ或はリニアライス抵抗等の温度一抵抗値変
化体Rtはそれぞれ並列に接続されており、そえぞれ同
一雰囲気内に設置してある。湿度一抵抗値変化体Rhに
は直流分阻用コンデンサーCのローパスフィルタを直列
に接続する事によつて湿度一抵抗値変化体の分極作用を
防止してある。電源切換時におこるオフセット電圧によ
つて温度一抵抗値変化体Rhが分極作用を起こし、電荷
がたまつてセンサーを劣化させるのを防ぐためにコンデ
ンサーCが入れてある。温度一抵抗値変化体Rtには直
流のみを通す様にダイオードD等の整流素子を直列して
ある。In FIG. 1, a master station 10 is provided in a central monitoring section and is connected to a slave station 20 by two transmission lines rl and 2. In the master station 10, switches 51 and 52 are connected to the constant voltage power supply E.
The electric force is switched by a flip-flop circuit or the like so as to alternately apply the electric force to the slave station 20 in the opposite direction, and it is switched from the common terminals Cl and C2 to the terminals al and a2 side and bl and b2 side at equal time intervals. be. Rs is extraction terminal 1
This is a reference resistor connected between 1 and 12. In the slave station 20, a humidity-resistance variable body Rh such as an electrical resistance type humidity detector is used.
and a temperature-resistance variable body Rt such as a thermistor or a linear rice resistor are connected in parallel and placed in the same atmosphere. A low-pass filter of a DC blocking capacitor C is connected in series to the humidity/resistance variable body Rh to prevent polarization of the humidity/resistance variable body. A capacitor C is inserted to prevent the temperature-resistance variable body Rh from polarizing due to the offset voltage that occurs when switching the power supply, and from accumulating charges and deteriorating the sensor. A rectifying element such as a diode D is connected in series to the temperature-resistance variable body Rt so as to pass only direct current.
今電源Eより交互に等しい時間間隔で逆方向の電流が与
えられる時には、湿度一抵抗値変化体Rhには両方向の
電流が流れ、温度一抵抗値変化体Rtには一方向の電流
が流れる。今、スイツチSl,S2が端子Bl,b2側
に接続されると、伝送線r1に電流が流れ、湿度一抵抗
値変化体Rhに電流が流れる力人湿度一抵抗値変化体R
tには電流が流れない。Now, when currents in opposite directions are applied alternately from the power source E at equal time intervals, currents in both directions flow through the humidity/resistance variable body Rh, and current flows in one direction through the temperature/resistance variable body Rt. Now, when the switches Sl and S2 are connected to the terminals Bl and b2, a current flows through the transmission line r1, and a current flows through the humidity-resistance variable body Rh.
No current flows through t.
この時親局における基準抵抗Rsの両端子11,12に
表われる出力電圧V。lは下式で表わす事ができる。但
しRhは湿度一抵抗値変化体Rhの抵抗値であり、rは
伝送線Rl,r2のそれぞれの抵抗値で共に等しいもの
とする。At this time, an output voltage V appears at both terminals 11 and 12 of the reference resistor Rs in the master station. l can be expressed by the following formula. However, Rh is the resistance value of the humidity-resistance value variable body Rh, and r is the resistance value of each of the transmission lines Rl and r2, which are both equal.
他の記号もそれぞれの値を示すものとする。なお(1)
式成立のためにRh》Rs》2rの関係を満足するもの
とする。Other symbols also indicate their respective values. Note (1)
In order to establish the formula, it is assumed that the relationship Rh》Rs》2r is satisfied.
湿度一抵抗値変化体Rhの抵抗値は通常50キロオーム
内至1タグオーム程度の範囲で湿度変化にともない変化
するが、基準抵抗Rsの抵抗値は200オーム程度であ
り、伝送線抵抗rは10オーム程度である。The resistance value of the humidity-resistance value variable body Rh usually changes with changes in humidity within the range of 50 kilohms to about 1 tag ohm, but the resistance value of the reference resistor Rs is about 200 ohms, and the transmission line resistance r is 10 ohms. That's about it.
湿度一抵抗値変化体Rhが第5図に示すように相対湿度
(%)の対数函数として示され、またこの値は温度をパ
ラメータにとつており、温度上昇にともない同一の相対
湿度では抵抗値が低い値となる。これを第6図に示す様
に抵抗値Rhの逆数(Qh)を縦軸にとつ碧時、値Qh
は相対湿度に対しほぼ比例関係にある。また温度上昇が
あれば値Qhも変化し、この割合は第7図に示す様にほ
ぼ温度上昇に対して比例した関係となる。ここで、値R
hに替えその逆数Qhを(1)式に入れると、値Qhは
温度依存性及び基準湿度での基準アドミツタンスQhs
があるために更に下式として示される。The humidity-resistance value changing body Rh is shown as a logarithmic function of relative humidity (%) as shown in Figure 5, and this value takes temperature as a parameter, and as the temperature rises, the resistance value changes at the same relative humidity. has a low value. As shown in Figure 6, when the reciprocal of the resistance Rh (Qh) is plotted on the vertical axis, the value Qh
is approximately proportional to relative humidity. Further, if the temperature rises, the value Qh also changes, and this ratio is approximately proportional to the temperature rise, as shown in FIG. Here, the value R
If we replace h with its reciprocal Qh in equation (1), the value Qh becomes the standard admittance Qhs at the temperature dependence and standard humidity.
Since there is, it is further shown as the following formula.
一方、スイツチSl,S2が端子Al,a2側に切換え
られれば電流は逆方向となり、伝送線Rl,r2に電流
1が湿度一抵抗値変化体Rhに電流11が流れるとする
と温度抵抗値変化体Rtにはl−11が流れる。On the other hand, if the switches Sl and S2 are switched to the terminals Al and a2, the current will flow in the opposite direction, and if current 1 flows through the transmission lines Rl and r2 and current 11 flows through the humidity-resistance value changing body Rh, then the temperature resistance value changing body l-11 flows through Rt.
この時下式が成立する。At this time, the following formula holds true.
但しVdはダイオードDの順方向電圧
但しコンデンサーCのインピーダンスRcはf−10H
z1C−500μFとするとz−±)
−2πFcl.5キロオームとなり、Rh>l
>Rcとなり無視する事ができる。However, Vd is the forward voltage of diode D. However, the impedance Rc of capacitor C is f-10H.
If z1C-500μF, then z-±)
−2πFcl. 5 kiloohm, Rh>l
>Rc and can be ignored.
(5)式は次式に変換する事ができる。Equation (5) can be converted into the following equation.
(6)式を(4)式に代入して、
この時の基準抵抗Rsの両端に表われる出力電圧02は
次式で示される。Substituting equation (6) into equation (4), the output voltage 02 appearing across the reference resistor Rs at this time is expressed by the following equation.
但し、2r<RsくRtくRhとする事が可能である。However, it is possible to set 2r<Rs x Rt x Rh.
ここで、Rtは第8図に示す様に温度の対数函数である
、また第9図の如く温度一可変抵抗体Rtの逆数をQt
が温度に対して後述する理由で比例関係にあるとする事
ができる場合に於ては次式が成立する。また値Qtは基
準アドミツタンスQts
VO2−1:(E−Vd)Rs−Qt=(E−Vd)R
s(△Qt+Qts)二(E−Vd)Rs・△Qt+(
E−Vd)Rs−Qts・・・(代)今、例えばサーミ
スターの抵抗値Rtは温度の対数函数であり、このサー
ミスターに直列抵抗を入れ、両者の逆数即ち、Qtを用
いると温度の一次比例函数として表わす事ができる。Here, Rt is a logarithmic function of temperature as shown in Fig. 8, and as shown in Fig. 9, Qt is the reciprocal of temperature - variable resistor Rt.
If it can be assumed that there is a proportional relationship to temperature for the reason described later, the following equation holds true. Also, the value Qt is the standard admittance Qts VO2-1: (E-Vd)Rs-Qt=(E-Vd)R
s(△Qt+Qts)2(E-Vd)Rs・△Qt+(
E-Vd) Rs-Qts...(V) Now, for example, the resistance value Rt of a thermistor is a logarithmic function of temperature.If you insert a series resistance into this thermistor and use the reciprocal of both, that is, Qt, the temperature It can be expressed as a linear proportional function.
以上によると一定の周波数で定電圧電源Eの極性を交互
に逆転し、第2図に示す様に出力電圧VOlVO2が零
を基準に波高値となつて基準抵抗Rsの両端に表われる
。According to the above, the polarity of the constant voltage power supply E is alternately reversed at a constant frequency, and as shown in FIG. 2, the output voltage VO1VO2 has a peak value with respect to zero and appears at both ends of the reference resistor Rs.
(3)式を適当なる常数KによりK倍すると、K−E−
Rs・△Qt2=(E−Vd)Rs・△Qtなる条件を
満足する様にした時、(自)式と(自)式を引算演算し
、下式を得る。When formula (3) is multiplied by K by an appropriate constant K, K-E-
When the condition Rs.ΔQt2=(E-Vd)Rs.ΔQt is satisfied, the following equation is obtained by subtracting the (self) equation and the (own) equation.
但し△Hは相対湿度、cは定数、Kは係数(自)式の結
果は温度に依存する湿度センサーを使用し、温度センサ
ーを媒体として、温度に依存しない真の相対湿度に比例
した出力oを得る事ができるものである。However, △H is the relative humidity, c is a constant, and K is a coefficient.The result of the formula uses a temperature-dependent humidity sensor, and the temperature sensor is used as a medium, and the output o is proportional to the true relative humidity that is independent of temperature. This is something that can be obtained.
第4図に本発明の一実施例の具体的回路図を示す。FIG. 4 shows a specific circuit diagram of an embodiment of the present invention.
第4図の上側回路は親局における子局への供給電圧の極
性を切換えて与える回路であり、下側回路は、基準抵抗
Rsの両端に表われる出力VOから温度に依存しない真
の湿度に比例した出力電圧V。3を得るための回路であ
る。The upper circuit in Figure 4 is a circuit that switches the polarity of the voltage supplied to the slave stations in the master station, and the lower circuit converts the output VO appearing across the reference resistor Rs to the true humidity independent of temperature. Proportional output voltage V. This is a circuit to obtain 3.
第3図におけるA,B,C,D,Eの各グラソは第4図
におけるA,B.C,D,E点における電圧値を示すも
のであり、A点は湿度一抵抗値変化体Rhに生じる出力
電圧を増巾器を経てK倍された値として(自)式の結果
を示すものである。Each glasso of A, B, C, D, E in FIG. 3 corresponds to A, B. in FIG. 4. It shows the voltage values at points C, D, and E, and point A shows the result of formula (self) as the value obtained by multiplying the output voltage generated in the humidity-resistance variable body Rh by K through the amplifier. It is.
B点は温度一抵抗値変化体Rtに生じる電圧V。2を示
し、C点D点ではA,B点における平滑された値であり
、E点はC点D点における出力の引算演算された(自)
式で示される電圧V。Point B is the voltage V generated across the temperature-resistance variable body Rt. 2, and point C and D are the smoothed values at points A and B, and point E is the result of the subtraction operation of the output at point C and D.
The voltage V shown by the formula.
3として表われる。Appears as 3.
以上の様に本発明は二線によつて湿度に依存しない真の
相対湿度値を得る事ができるもので、二線の伝送線のみ
で良い事及び電源を子局側に設ける必要のない事によつ
て得られる経済的利益はきわめて大きい。As described above, the present invention is capable of obtaining a true relative humidity value independent of humidity using two wires, and only requires two transmission lines, and there is no need to provide a power source on the slave station side. The economic benefits that can be gained from this are extremely large.
図は本発明実施例で、第1図は原理説明のための回路結
線図、第4図は具体的な回路結線図、第2図及び第3図
は出力電圧の特性図、第5図は相対湿度%Rhと温度一
抵抗値変化体の抵抗値Rhとの関係を示すグラフ、第6
図は抵抗値Rhの逆数Qhの異る温度状態における相対
湿度%Rhとの関係を示すグラフ、第7図は逆数Qhと
温度℃との関係を示すグラフ、第8図は温度一抵抗値変
化体の抵抗値Rtと温度℃との関係を示すグラフ、第9
図は抵抗値Rtの逆数Qtと温度との関係を示すグラフ
である。
10・・・・・・親局、20・・・・・・子局、Rh・
・・・・・湿度一抵抗値変化体、Rt・・・・・・温度
一抵抗値変化体、Rs・・・・・・基準抵抗、Sl,S
2・・・・・・切換スイツチ、F・・・・・・フリツプ
ロツプ回路。The figures show an embodiment of the present invention, Fig. 1 is a circuit connection diagram for explaining the principle, Fig. 4 is a concrete circuit connection diagram, Figs. 2 and 3 are output voltage characteristic diagrams, and Fig. 5 is a circuit connection diagram for explaining the principle. Graph showing the relationship between relative humidity %Rh and resistance value Rh of the temperature-resistance value changing body, No. 6
The figure is a graph showing the relationship between the reciprocal Qh of the resistance value Rh and the relative humidity %Rh in different temperature conditions. Figure 7 is a graph showing the relationship between the reciprocal Qh and the temperature °C. Figure 8 is the change in temperature vs. resistance value. Graph showing the relationship between body resistance value Rt and temperature °C, No. 9
The figure is a graph showing the relationship between the reciprocal Qt of the resistance value Rt and temperature. 10... Master station, 20... Slave station, Rh.
...Humidity - resistance value changing body, Rt...temperature - resistance value changing body, Rs ......standard resistance, Sl, S
2... Changeover switch, F... flipflop circuit.
Claims (1)
ーパスフィルターが、直列接続された温度−抵抗値変化
体とダイオードに並列接続され、親局は極性を変化させ
て電圧を与える電源およびその電源と直列に接続された
基準抵抗を有しており、2本の伝送線に並列接続された
子局へ親局から2本の伝送線を介して交互に逆方向の電
圧が与えられ、親局では基準抵抗の両端に発生した相対
湿度および温度に依存した電圧と、温度に依存した電圧
とを引算演算することによつて温度に依存しない相対湿
度を得るようにした二線式湿度計測伝送装置。1 In the slave station, a series-connected humidity-resistance variable body and a low-pass filter are connected in parallel to a series-connected temperature-resistance variable body and a diode, and the master station connects a power source and a voltage source that change the polarity to provide voltage. It has a reference resistor connected in series with the power supply, and voltages in opposite directions are alternately applied from the master station to the slave stations connected in parallel to the two transmission lines via the two transmission lines. At the master station, the two-wire humidity system obtains temperature-independent relative humidity by subtracting the relative humidity and temperature-dependent voltage generated across the reference resistor and the temperature-dependent voltage. Measurement transmission equipment.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP50116934A JPS592080B2 (en) | 1975-09-27 | 1975-09-27 | Nisenshikisitsudohatsushinki |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP50116934A JPS592080B2 (en) | 1975-09-27 | 1975-09-27 | Nisenshikisitsudohatsushinki |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5240359A JPS5240359A (en) | 1977-03-29 |
| JPS592080B2 true JPS592080B2 (en) | 1984-01-17 |
Family
ID=14699306
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP50116934A Expired JPS592080B2 (en) | 1975-09-27 | 1975-09-27 | Nisenshikisitsudohatsushinki |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS592080B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB2234069B (en) * | 1988-10-28 | 1992-08-12 | Motorola Inc | Sensor arrangement |
| US7265560B2 (en) * | 2005-11-23 | 2007-09-04 | Therm-O-Disc, Incorporated | Temperature compensated vapor sensor |
| JP6766352B2 (en) * | 2015-12-15 | 2020-10-14 | ブラザー工業株式会社 | Interface circuit |
-
1975
- 1975-09-27 JP JP50116934A patent/JPS592080B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5240359A (en) | 1977-03-29 |
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