JPH0713626B2 - Magnetic oximeter - Google Patents
Magnetic oximeterInfo
- Publication number
- JPH0713626B2 JPH0713626B2 JP62327916A JP32791687A JPH0713626B2 JP H0713626 B2 JPH0713626 B2 JP H0713626B2 JP 62327916 A JP62327916 A JP 62327916A JP 32791687 A JP32791687 A JP 32791687A JP H0713626 B2 JPH0713626 B2 JP H0713626B2
- Authority
- JP
- Japan
- Prior art keywords
- purge gas
- magnetic field
- bypass pipe
- output
- detection
- 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 - Lifetime
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- Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)
Description
【発明の詳細な説明】 <産業上の利用分野> 本発明は、酸素ガスの磁気的性質を利用して測定ガス中
の酸素ガス濃度を検出する磁気式酸素計に関する。TECHNICAL FIELD The present invention relates to a magnetic oximeter that detects the oxygen gas concentration in a measurement gas by utilizing the magnetic properties of oxygen gas.
<従来の技術> 磁気式酸素計は、酸素ガスの磁化率が他のガスに比べて
非常に大きく、この性質を利用して測定ガス中の酸素濃
度を測定する分析計である。本件出願人は特願昭第60−
161601号によって第5図に示す独特な磁気式酸素計を提
案した。<Prior Art> A magnetic oximeter is an analyzer that measures the oxygen concentration in a measurement gas by utilizing this property, because the magnetic susceptibility of oxygen gas is much larger than that of other gases. The applicant of the present application is Japanese Patent Application No. 60-
We proposed a unique magnetic oximeter shown in Fig. 5 by 161601.
図中、一点鎖線で囲んだ部分1は検出部、2は変換部で
ある。SCは検出部1に収容された測定セルで、このうち
101は測定室を形成する閉ループ状測定通路、102,103は
測定通路101の対称位置に設けられた測定ガスSg用の入
口と出口、104は入口102と出口103との中間部に設けら
れた、二つの円弧状測定通路部分を接続するバイパス
管、105はこのバイパス管の中央に設けられたパージガ
スPgの導入口である。またバイパス管104と測定通路101
との接続部分A,Bのうち一方の接続部分Aには、例えば
永久磁石を用いた磁界(Mf)形成手段が設けられてい
る。In the figure, a part 1 surrounded by a one-dot chain line is a detection part, and 2 is a conversion part. SC is a measurement cell housed in the detection unit 1, of which
101 is a closed loop measurement passage forming a measurement chamber, 102 and 103 are inlets and outlets for the measurement gas Sg provided at symmetrical positions of the measurement passage 101, and 104 is provided at an intermediate portion between the inlet 102 and the outlet 103. A bypass pipe that connects the two arc-shaped measurement passage portions, and 105 is an inlet for the purge gas Pg provided at the center of the bypass pipe. Also, bypass pipe 104 and measurement passage 101
A magnetic field (Mf) forming means using, for example, a permanent magnet is provided at one of the connecting portions A and B of the connecting portions A and B.
106,107はバイパス管104においてパージガス導入口105
を挾んで対称位置に設けられたパージガス流検出用測温
抵抗センサで、例えばサーミスタ等、抵抗値温度係数の
大きなセンサが用いられる。Reference numerals 106 and 107 denote purge gas inlets 105 in the bypass pipe 104.
A temperature-measuring resistance sensor for detecting a purge gas flow, which is provided in a symmetrical position with a large temperature coefficient of resistance such as a thermistor.
変換部2において、201,202はセンサ106,107に夫々接続
された温度制御回路、203はこれらの出力の差をとる引
算回路である。温度制御回路201,202はセンサ106,107の
熱的応答の遅れを無くすためセンサの温度を一定に制御
する回路である。In the conversion unit 2, 201 and 202 are temperature control circuits connected to the sensors 106 and 107, respectively, and 203 is a subtraction circuit that takes the difference between these outputs. The temperature control circuits 201 and 202 are circuits that control the temperature of the sensors 106 and 107 to be constant in order to eliminate the delay in the thermal response of the sensors 106 and 107.
このような構成で、測定ガスSg中に酸素ガスが含まれて
いない場合、磁界Mfへの酸素ガスの吸引はないから、バ
イパス管104において接続部分A及びBに向かって分流
されるパージガスQL,QR流速には変化はない。一方、測
定ガスSgに酸素ガスが含まれている場合、磁界Mfへの酸
素ガスの吸引が起こり、矢印QOの酸素ガスの流れが生
じ、この結果、QLの流速は減少し、QRの流速が増大す
る。With such a configuration, when the measurement gas Sg does not contain oxygen gas, the oxygen gas is not sucked into the magnetic field Mf, so the purge gas Q L diverted toward the connection portions A and B in the bypass pipe 104. , change in the flow rate Q R is not. On the other hand, when the measurement gas Sg contains oxygen gas, the suction of oxygen gas to the magnetic field Mf occurs, and the flow of oxygen gas at the arrow Q O occurs, and as a result, the flow velocity of Q L decreases and Q R The flow rate of
バイパス管104を分流するパージガスQL,QRの流速の変化
は測定ガスSg中の酸素濃度に対応しており、測温抵抗セ
ンサ106,107の抵抗値変化からこれを検出する。尚、こ
れらセンサの抵抗値はパージガスQL,QRの流速に応じて
変化するが温度制御回路201,202から帰還が掛かり、セ
ンサ106,107の電源電圧を変化させ、これらセンサの温
度、即ち抵抗値が一定になるように制御される。The change in the flow velocity of the purge gases Q L and Q R diverting the bypass pipe 104 corresponds to the oxygen concentration in the measurement gas Sg, which is detected from the change in the resistance value of the temperature measuring resistance sensors 106 and 107. The resistance values of these sensors change according to the flow rates of the purge gases Q L and Q R , but feedback is applied from the temperature control circuits 201 and 202 to change the power supply voltage of the sensors 106 and 107, and the temperature of these sensors, that is, the resistance value is constant. Controlled to be.
これら帰還信号の大きさは、パージガスQL,QRの流速に
対応しており、温度制御回路201,202の出力信号VR,VLと
して引算回路203に与えられ、この回路においてこれら
の差がとられ、出力信号VOとして出力される。The magnitude of these feedback signals, the purge gas Q L, corresponds to the flow rate of Q R, the output signal V R of the temperature control circuit 201 is given to the subtraction circuit 203 as V L, these differences in the circuit And is output as an output signal V O.
このような装置の場合、センサ106,107がパージガスQL,
QRが常時流れている管路中に置かれている為、信号分の
大きな検出出力が得られる利点があり、更に、引算回路
203でセンサ106,107の検出出力の差がとられるため、外
部からの衝撃や振動に対し強い利点がある。In the case of such an apparatus, the sensors 106 and 107 are the purge gas Q L ,
Since Q R is placed in the pipe flowing constantly, there is the advantage that a large detection output signal component is obtained, further, subtraction circuit
Since the difference between the detection outputs of the sensors 106 and 107 is taken by 203, there is a strong advantage against external impact or vibration.
<発明が解決しようとする問題点> しかしながら、センサ106,107の検出出力とパージガスQ
L,QRの流量(流速)とは非直線な関係にあり、パージガ
スQL,QRの流量が変った場合に、単純にセンサ106,107の
検出出力の差をとっただけでは測定誤差を引起こす。<Problems to be Solved by the Invention> However, the detection outputs of the sensors 106 and 107 and the purge gas Q
L, is in the non-linear relationship between the flow rate of Q R (flow rate), the purge gas Q L, when the flow rate of Q R has changed, by simply just took the difference between the detection output of the sensor 106 and 107 pull the measurement error Wake up.
更に測定ガスSg中にH2,Heガスが含まれている場合、こ
れらガスは他のガスに比べて拡散係数が大きく、接続部
分A,BからのパージガスPgの流出に逆らってバイパス管1
04内に入り込む。このようなガスの拡散によりバイパス
管104内には温度分布が発生し、センサ106,107に熱的な
影響を与えて出力誤差を発生させる。Further, when the measurement gas Sg contains H 2 and He gases, these gases have a larger diffusion coefficient than other gases, and the bypass pipe 1 is provided against the outflow of the purge gas Pg from the connection portions A and B.
04 Enter inside. Due to such gas diffusion, a temperature distribution is generated in the bypass pipe 104, which has a thermal effect on the sensors 106 and 107 and causes an output error.
本発明において解決しようとする第1の技術的課題は、
前述の磁気式酸素において、前記センサの非直線特性の
影響が検出結果に現れないようにすることにあり、第2
の技術的課題は前記測定ガス中に含まれる拡散係数の大
きなガス成分の影響を受けないようにすることにある。The first technical problem to be solved in the present invention is
In the above-mentioned magnetic oxygen, it is to prevent the influence of the non-linear characteristic of the sensor from appearing in the detection result.
The technical problem of (1) is to prevent the influence of a gas component having a large diffusion coefficient contained in the measurement gas.
<問題点を解決するための手段> 本発明の第1の発明の構成は、閉ループ状の測定通路の
対称位置に測定ガス用入口と出口とを設け、これら入口
と出口の中間位置にバイパス管を接続し、このバイパス
管の中央にパージガス導入口を設けた測定室と、前記バ
イパス管と前記閉ループ状測定通路の接続部分の一方に
設けた磁界形成手段と、前記パージガス導入口を挟んで
対称位置に設けられ前記バイパス管中に配置された一対
のパージガス流検出用測温抵抗センサからなる検出部
と、前記パージガスの流量がゼロの状態における前記一
対のセンサからの出力と前記パージガスを流した状態に
おける前記一対のセンサからの出力を取り込んでゼロ誤
差の差し引き補正を行うと共に VO=K{VR−VRO)1/2−(VL−VLO)1/2} 但し、 VR:非磁界側のセンサの検出出力 VRO:パージガス流量がゼロのときの非磁界側のセンサの
検出出力 VL:磁界側のセンサの検出出力 VLO:パージガス流量がゼロのときの磁界側のセンサの検
出出力 K :定数 の式に基づいて非直線関係の影響を除去した信号を出力
する演算手段からなる変換部とを具備するものであり、 本発明の第2の発明の構成は、閉ループ状の測定通路の
対称位置に測定ガス用入口と出口とを設け、これら入口
と出口の中間位置にバイパス管を接続し、このバイパス
管の中央にパージガス導入口を設けた測定室と、前記バ
イパス管と前記閉ループ状測定通路の接続部分の一方に
設けた磁界形成手段と、前記パージガス導入口を挟んで
対称位置に設けられ前記バイパス管中に配置された一対
の絞りと、この絞りと前記パージガス導入口を挟んで対
称位置に設けられたパージガス流検出用測温抵抗センサ
からなる検出部と、前記パージガスの流量がゼロの状態
における前記一対のセンサからの出力と前記パージガス
を流した状態における前記一対のセンサからの出力を取
り込んでゼロ誤差の差し引き補正を行うと共に VO=K{VR−VRO)1/2−(VL−VLO)1/2} 但し、 VR:非磁界側のセンサの検出出力 VRO:パージガス流量がゼロのときの非磁界側のセンサの
検出出力 VL:磁界側のセンサの検出出力 VLO:パージガス流量がゼロのときの磁界側のセンサの検
出出力 K :定数 の式に基づいて非直線関係の影響を除去した信号を出力
する演算手段からなる変換部とを具備したことにある。<Means for Solving the Problems> In the configuration of the first invention of the present invention, a measurement gas inlet and an outlet are provided at symmetrical positions of a closed loop measurement passage, and a bypass pipe is provided at an intermediate position between these inlet and outlet. And a measuring chamber having a purge gas inlet at the center of the bypass pipe, a magnetic field forming means provided at one of the connecting portions of the bypass pipe and the closed loop measurement passage, and the purge gas inlet being symmetrical. A detection unit including a pair of temperature-measuring resistance sensors for purge gas flow detection provided in a position and arranged in the bypass pipe, and output from the pair of sensors and the purge gas when the flow rate of the purge gas is zero. V O = K performs subtraction correction of the zero error takes in the output from said pair of sensors in a state {V R -V RO) 1/2 - (V L -V LO) 1/2} where, V R : Non magnetic field Sensor detection output V RO: purge flow detection output V of the non-magnetic side sensor when zero L: detection output V LO magnetic field side of the sensor: the detection output of the magnetic field of the sensor when the purge gas flow rate is zero K: a constant value, and a conversion unit configured to output a signal in which the influence of the non-linear relation is removed based on the equation, and the configuration of the second invention of the present invention is a closed loop measurement passage. A measurement gas inlet and an outlet are provided at symmetrical positions, a bypass pipe is connected to an intermediate position between the inlet and the outlet, and a purge gas introduction port is provided in the center of the bypass pipe, the bypass pipe and the closed loop. Field forming means provided on one side of the connection portion of the shape measuring passage, a pair of throttles arranged symmetrically across the purge gas introduction port and arranged in the bypass pipe, and this throttle and the purge gas introduction port are sandwiched. And a detection unit comprising a temperature measuring resistance sensor for purge gas flow detection provided at symmetrical positions, the output from the pair of sensors when the flow rate of the purge gas is zero, and the pair of sensors when the purge gas is flowing. V O = K {V R -V RO) 1/2 - (V L -V LO) 1/2} performs subtraction correction of the zero error takes in the output of the proviso, V R: the non-magnetic side sensor Detection output V RO : Detection output of non-magnetic field side sensor when purge gas flow rate is zero VL : Detection output of magnetic field side sensor V LO : Detection output of magnetic field side sensor when purge gas flow rate is zero K: Constant And a conversion unit including a calculation unit that outputs a signal in which the influence of the non-linear relation is removed based on the equation (1).
<作用> 前記第1の発明は次のように作用する。即ち、先ず、前
記パージガス流量がゼロの状態で前記一対のセンサで検
出されるゼロ誤差信号を記憶し、次に、前記パージガス
を流した状態で検出を行い検出信号から前記ゼロ誤差信
号を差引き、ゼロ補償された信号出力を得る。<Operation> The first aspect of the present invention operates as follows. That is, first, the zero error signal detected by the pair of sensors is stored when the purge gas flow rate is zero, and then the detection is performed with the purge gas flowing, and the zero error signal is subtracted from the detection signal. , Get a zero compensated signal output.
前記パージガス流量と前記センサの検出信号との非直線
関係は予め分かっており、この非直線関係式に基づき非
直線補正演算を行い、これら非直線補正された信号の差
を取ることにより前記センサの非直線特性の影響を受け
ない酸素ガス濃度信号を得る。The non-linear relationship between the purge gas flow rate and the detection signal of the sensor is known in advance, a non-linear correction calculation is performed based on this non-linear relational expression, and the difference between these non-linearly corrected signals is taken to obtain the sensor An oxygen gas concentration signal that is not affected by nonlinear characteristics is obtained.
前記第2の発明は前記第1の発明の作用に加え、次のよ
うに作用する。即ち、前記測定ガスに含まれる拡散係数
の大きなガスは、前記閉ループ状測定通路との接続部分
から前記センサに向かって指数関数的な濃度分布を持
ち、前記センサ部分における拡散ガスの濃度は前記パー
ジガスの流速が大きい程低くなる。In addition to the operation of the first invention, the second invention operates as follows. That is, the gas with a large diffusion coefficient contained in the measurement gas has an exponential concentration distribution from the connection portion with the closed loop measurement passage toward the sensor, and the concentration of the diffusion gas in the sensor portion is the purge gas. The higher the flow velocity of, the lower.
本発明では、前記パージガス導入口を挾んで一対の絞り
を設け、前記パージガスの流速を大きくして前記センサ
部分における拡散ガスの濃度を下げ、前記測定ガスの組
成の影響が測定結果に現れないようにしている。In the present invention, a pair of throttles are provided across the purge gas introduction port to increase the flow velocity of the purge gas to reduce the concentration of the diffusion gas in the sensor portion so that the influence of the composition of the measurement gas does not appear in the measurement result. I have to.
<実施例> 以下図面に従い本発明の実施例を説明する。第1図は本
発明実施例装置の全体構成を示すブロック線図である。
第2図は本発明実施例装置における測定セルを示し、図
(a)はその平面図、図(b)は図(a)におけるCDE
断面図である。これらの図中、第5図における要素と実
質的に同じ要素には同一符号を付しこれらについての説
明は省略する。先ず、第1図において、検出部1は恒温
槽になっており、測定ガスSgはフィルタ108、絞り109を
経て測定セルSCに与えられる。パージガスPgはフィルタ
110、キャピラリ111を通り測定セルSCに与えられる。11
2は磁界を発生させる磁石、113は検出回路、114は温度
検出素子、115はヒータである。<Example> An example of the present invention will be described below with reference to the drawings. FIG. 1 is a block diagram showing the overall configuration of the apparatus of the present invention.
FIG. 2 shows a measuring cell in an apparatus of the present invention, FIG. 2A is a plan view thereof, and FIG. 2B is a CDE in FIG.
FIG. In these figures, elements that are substantially the same as the elements in FIG. 5 are assigned the same reference numerals and explanations thereof are omitted. First, in FIG. 1, the detection unit 1 is a thermostatic chamber, and the measurement gas Sg is supplied to the measurement cell SC through the filter 108 and the diaphragm 109. Purge gas Pg is a filter
It is given to the measuring cell SC through 110 and the capillary 111. 11
2 is a magnet for generating a magnetic field, 113 is a detection circuit, 114 is a temperature detection element, and 115 is a heater.
測定セルSC部分について第2図に従い詳しく説明する。
測定セルSCは外側のリング116と内側のディスク117の二
つの部分から構成されている。閉ループを形成するリン
グ状測定通路101はディスク117の外周に設けられた溝を
リング116で封止する形で形成されている。測定ガスSg
の入口102と出口103とはディスク117の上面でリング状
測定通路101より内側になるように設けられている。磁
石112はディスク117に埋め込まれている。118と119はバ
イパス管104においてパージガス導入口105を挾んで対称
位置に設けられた絞りである。The measuring cell SC portion will be described in detail with reference to FIG.
The measuring cell SC consists of two parts, an outer ring 116 and an inner disc 117. The ring-shaped measuring passage 101 forming a closed loop is formed by sealing a groove provided on the outer periphery of the disk 117 with a ring 116. Measuring gas Sg
The inlet 102 and the outlet 103 are provided on the upper surface of the disk 117 so as to be inside the ring-shaped measurement passage 101. The magnet 112 is embedded in the disk 117. Reference numerals 118 and 119 are throttles provided at symmetrical positions in the bypass pipe 104 with the purge gas introduction port 105 interposed therebetween.
第1図に戻り、変換部2内において、204はマルチプレ
クサでここで選択された検出回路113の出力はA/D変換回
路205によりデジタル量に変換され、入・出力ポート206
を経てマイクロプロセッサ207に取りこまれる。一方、
温度検出素子114で検出された信号も検出回路113、A/D
変換回路205、入・出力ポート206を経てマイクロプロセ
ッサ207に取りこまれ、ヒータ駆動回路208に温度制御信
号が与えられヒータ115が駆動されて、温度制御され
る。尚、209は演算プログラム等が格納されたROM、210
は表示・キー部、211は出力回路である。Returning to FIG. 1, in the conversion unit 2, 204 is a multiplexer, and the output of the detection circuit 113 selected here is converted into a digital amount by the A / D conversion circuit 205, and the input / output port 206
Then, it is taken in by the microprocessor 207. on the other hand,
The signal detected by the temperature detection element 114 is also detected by the detection circuit 113, A / D
It is taken into the microprocessor 207 via the conversion circuit 205 and the input / output port 206, and a temperature control signal is given to the heater drive circuit 208 to drive the heater 115 to control the temperature. In addition, 209 is a ROM in which a calculation program is stored, 210
Is a display / key unit, and 211 is an output circuit.
次に、このように構成された装置の動作について説明を
行う。先ず、測定に先立ちパージガスPgがゼロの状態で
センサ106,107によって検出を行い、このときの検出出
力をゼロ誤差信号としてマイクロプロセッサ206中に記
憶させる。次いで、パージガスPgを流して測定を行い、
そのとき検出された検出信号から前記ゼロ誤差信号を差
引きゼロ補正を行う。Next, the operation of the apparatus thus configured will be described. First, prior to the measurement, detection is performed by the sensors 106 and 107 while the purge gas Pg is zero, and the detection output at this time is stored in the microprocessor 206 as a zero error signal. Then, the purge gas Pg is flowed to perform the measurement,
The zero error signal is subtracted from the detection signal detected at that time to perform zero correction.
パージガスPgの流量とセンサ106,107の検出出力とは非
直線の関係にあり、その関係は予め分かっている。例え
ば前記検出信号がパージガス流量に対し第3図に示すよ
うな2乗特性を有しているような場合、 VO=K{(VR−VRO)1/2−(VL−VLO)1/2} …(1) なる演算を行い、センサ106,107の非直線特性の影響を
受けない酸素ガス濃度出力VOを得ている。The flow rate of the purge gas Pg and the detection outputs of the sensors 106 and 107 have a non-linear relationship, and the relationship is known in advance. For example, when the detection signal has a squared characteristic as shown in FIG. 3 with respect to the purge gas flow rate, V O = K {(V R −V RO ) 1/2 − (V L −V LO ) 1/2 } (1) is calculated to obtain the oxygen gas concentration output V O that is not affected by the nonlinear characteristics of the sensors 106 and 107.
(但し、VL:磁界側のセンサ106の検出出力、 VR:非磁界側のセンサ107の検出出力、 VLO:パージガス流量がゼロのときの磁界側のセンサ106
の検出出力、VRO:パージガス流量がゼロのときの非磁界
側のセンサ107の検出出力、K:定数) 一方、測定ガスSgに拡散係数の大きなH2,Heガスが含ま
れているとき、接続部分A,BからパージガスPgの流出に
逆らってバイパス管104内にこれら拡散ガスは入り込
む。この拡散ガスは接続部分A,Bからセンサ106,107に向
かって指数関数的濃度分布を持ち、センサ106,107部分
において次式で示すような濃度CN(X)を持つ。(However, V L : detection output of the magnetic field side sensor 106, V R : detection output of the non-magnetic field side sensor 107, V LO : magnetic field side sensor 106 when the purge gas flow rate is zero
Detection output, V RO : detection output of the sensor 107 on the non-magnetic field side when the purge gas flow rate is zero, K: constant) On the other hand, when the measurement gas Sg contains H 2 and He gas with a large diffusion coefficient, These diffusion gases enter the bypass pipe 104 against the outflow of the purge gas Pg from the connection portions A and B. This diffusion gas has an exponential concentration distribution from the connecting portions A and B toward the sensors 106 and 107, and has a concentration C N (X) in the sensor 106 and 107 portions as shown by the following equation.
CN(X)=CNO・exp{−(V・X)/Dn} …(2) (但し、CNO:接続部分A或はBにおける拡散ガスの濃
度、V:パージガスPgの流速、X:接続部分A,Bからセンサ1
06,107迄の距離、Dn:拡散ガスの拡散係数) この式から分かるように、パージガスPgの流速Vを大き
くするか、或は接続部分A,Bからセンサ106,107迄の距離
Xを長くすれば、拡散の割合は指数的に小さくなる。C N (X) = C NO · exp {− (V · X) / Dn} (2) (where C NO : concentration of diffusion gas at connecting portion A or B, V: flow velocity of purge gas Pg, X : From connection A, B to sensor 1
(Distance to 06,107, Dn: Diffusion coefficient of diffusion gas) As can be seen from this equation, if the flow velocity V of the purge gas Pg is increased or the distance X from the connecting portions A and B to the sensors 106 and 107 is lengthened, diffusion will occur. The ratio of will decrease exponentially.
Xを長くする方法として、バイパス管104を直線的に長
くする方法はセルSC全体が大きくなってしまうため採用
できない。バイパス管104を第4図に示すように逆S字
或はS字形に形成し管路長を稼ぐ方法が考えられるが、
このような方法の場合管路抵抗が増え、加工が難しくな
る欠点がある。As a method of lengthening X, a method of linearly lengthening the bypass pipe 104 cannot be adopted because the entire cell SC becomes large. The bypass pipe 104 may be formed in an inverted S-shape or S-shape as shown in FIG. 4 to increase the pipe length.
In the case of such a method, there is a drawback that the conduit resistance increases and the processing becomes difficult.
一方、Vを大きくする方法として、パージガスPgの流量
を増やす方法が考えられるが、パージガスの消費を早め
て得策ではない。On the other hand, as a method of increasing V, a method of increasing the flow rate of the purge gas Pg can be considered, but it is not a good idea to expedite the consumption of the purge gas.
本発明では、パージガス導入口105を挾んで一対の絞り1
18,119を設け、これら絞り部でパージガスの流速を上
げ、拡散ガスの影響を小さくしている。In the present invention, the purge gas inlet 105 is sandwiched between the pair of throttles 1
18,119 are provided, and the flow velocity of the purge gas is increased at these throttles to reduce the influence of the diffusion gas.
<発明の効果> 本発明の第1の発明によれば、前述の磁気式酸素計にお
いて、前記センサの非直線特性の影響が検出結果に現れ
ない。また、本発明の第2の発明によれば、前記した効
果に加え、前記測定ガス中に含まれる前記拡散ガスの影
響が検出結果に現れない。<Effect of the Invention> According to the first invention of the present invention, in the above-described magnetic oximeter, the influence of the non-linear characteristic of the sensor does not appear in the detection result. Further, according to the second aspect of the present invention, in addition to the effects described above, the influence of the diffusion gas contained in the measurement gas does not appear in the detection result.
第1図は本発明実施例装置の全体構成を示すブロック線
図、第2図は本発明実施例装置における測定セルを示
し、図(a)はその平面図、図(b)はその断面図、第
3図、第4図は本発明実施例装置を説明するための説明
図、第5図は従来装置の構成図である。 1:検出部、2:変換部、101:測定通路、102:測定ガス用入
口、103:測定ガス用出口、104:バイパス管、105:パージ
ガス導入口、106,107:センサ、112:磁石、113:検出回
路、118,119:絞り、SC:測定セル、Mf:磁界、Sg:測定ガ
ス、Pg:パージガス、A,B……接続部分FIG. 1 is a block diagram showing the overall configuration of the device of the present invention, FIG. 2 shows a measuring cell in the device of the present invention, FIG. (A) is a plan view thereof, and FIG. (B) is a sectional view thereof. 3 and 4 are explanatory views for explaining the apparatus of the present invention, and FIG. 5 is a block diagram of a conventional apparatus. 1: detection part, 2: conversion part, 101: measurement passage, 102: measurement gas inlet, 103: measurement gas outlet, 104: bypass pipe, 105: purge gas inlet, 106, 107: sensor, 112: magnet, 113: Detection circuit, 118, 119: Aperture, SC: Measuring cell, Mf: Magnetic field, Sg: Measuring gas, Pg: Purge gas, A, B ... Connection part
───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 昭51−144295(JP,A) 特開 昭53−12674(JP,A) 特開 昭64−6753(JP,A) 特開 昭47−1250(JP,A) 特公 昭49−10280(JP,B1) 米国特許3471776(US,A) 米国特許3302448(US,A) ─────────────────────────────────────────────────── ─── Continuation of front page (56) References JP-A-51-144295 (JP, A) JP-A-53-12674 (JP, A) JP-A-64-6753 (JP, A) JP-A-47- 1250 (JP, A) Japanese Patent Publication No. Sho 49-10280 (JP, B1) US Patent 3471776 (US, A) US Patent 3302448 (US, A)
Claims (2)
ス用入口と出口とを設け、これら入口と出口の中間位置
にバイパス管を接続し、このバイパス管の中央にパージ
ガス導入口を設けた測定室と、前記バイパス管と前記閉
ループ状測定通路の接続部分の一方に設けた磁界形成手
段と、前記パージガス導入口を挟んで対称位置に設けら
れ前記バイパス管中に配置された一対のパージガス流検
出用測温抵抗センサからなる検出部と、前記パージガス
の流量がゼロの状態における前記一対のセンサからの出
力と前記パージガスを流した状態における前記一対のセ
ンサからの出力を取り込んでゼロ誤差の差し引き補正を
行うと共に下記の式に基づいて非直線関係の影響を除去
した信号を出力する演算手段からなる変換部とを具備す
る磁気式酸素計。 VO=K{(VR−VRO)1/2−(VL−VLO)1/2} 但し、 VR:非磁界側のセンサの検出出力 VRO:パージガス流量がゼロのときの非磁界側のセンサの
検出出力 VL:磁界側のセンサの検出出力 VLO:パージガス流量がゼロのときの磁界側のセンサの検
出出力 K :定数1. A measurement gas inlet and an outlet are provided at symmetrical positions of a closed loop measurement passage, a bypass pipe is connected to an intermediate position between the inlet and the outlet, and a purge gas inlet is provided at the center of the bypass pipe. A measurement chamber, a magnetic field forming means provided at one of the connecting portions of the bypass pipe and the closed loop-shaped measurement passage, and a pair of purge gas flows disposed in the bypass pipe at symmetrical positions with respect to the purge gas inlet. A detection unit consisting of a temperature measuring resistance sensor for detection, the output from the pair of sensors when the flow rate of the purge gas is zero and the output from the pair of sensors when the purge gas is flowing are taken in to subtract a zero error. A magnetic oximeter comprising: a conversion unit configured to perform correction and output a signal in which the influence of a non-linear relationship is removed based on the following equation. V O = K {(V R −V RO ) 1/2 − (V L −V LO ) 1/2 } where V R : Detection output of the non-magnetic field side sensor V RO : When the purge gas flow rate is zero Detection output of non-magnetic field side sensor V L : Detection output of magnetic field side sensor V LO : Detection output of magnetic field side sensor when purge gas flow rate is zero K: Constant
ス用入口と出口とを設け、これら入口と出口の中間位置
にバイパス管を接続し、このバイパス管の中央にパージ
ガス導入口を設けた測定室と、前記バイパス管と前記閉
ループ状測定通路の接続部分の一方に設けた磁界形成手
段と、前記パージガス導入口を挟んで対称位置に設けら
れ前記バイパス管中に配置された一対の絞りと、この絞
りと前記パージガス導入口を挟んで対称位置に設けられ
たパージガス流検出用測温抵抗センサからなる検出部
と、前記パージガスの流量がゼロの状態における前記一
対のセンサからの出力と前記パージガスを流した状態に
おける前記一対のセンサからの出力を取り込んでゼロ誤
差の差し引き補正を行うと共に下記の式に基づいて非直
線関係の影響を除去した信号を出力する演算手段からな
る変換部とを具備する磁気式酸素計。 記 VO=K{(VR−VRO)1/2−(VL−VLO)1/2} 但し、 VR:非磁界側のセンサの検出出力 VRO:パージガス流量がゼロのときの非磁界側のセンサの
検出出力 VL:磁界側のセンサの検出出力 VLO:パージガス流量がゼロのときの磁界側のセンサの検
出出力 K :定数2. A measuring gas inlet and an outlet are provided at symmetrical positions of a closed loop measuring passage, a bypass pipe is connected to an intermediate position between the inlet and the outlet, and a purge gas introducing port is provided at the center of the bypass pipe. A measurement chamber, a magnetic field forming means provided at one of the connecting portions of the bypass pipe and the closed loop-shaped measurement passage, and a pair of throttles provided at symmetrical positions across the purge gas introduction port and arranged in the bypass pipe. , A detection unit composed of a temperature measuring resistance sensor for purge gas flow detection, which is provided at a symmetrical position with the throttle gas and the purge gas introduction port interposed therebetween, and outputs from the pair of sensors and the purge gas when the flow rate of the purge gas is zero. The output from the pair of sensors in the state of flowing the current is taken in to perform the subtraction correction of the zero error, and the influence of the non-linear relation is removed based on the following formula. Magnetic oxygen analyzer comprising a conversion unit comprising a calculation means for outputting a signal. Serial V O = K {(V R -V RO) 1/2 - (V L -V LO) 1/2} where, V R: detection output V RO of the non-magnetic side sensor: When the purge gas flow rate is zero Output of non-magnetic field side sensor of V L : Detection output of magnetic field side sensor V LO : Detection output of magnetic field side sensor when purge gas flow rate is zero K: Constant
Priority Applications (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62327916A JPH0713626B2 (en) | 1987-12-24 | 1987-12-24 | Magnetic oximeter |
| US07/209,431 US4860574A (en) | 1987-06-29 | 1988-06-21 | Paramagnetic oxygen analyzer |
| DE3821979A DE3821979A1 (en) | 1987-06-29 | 1988-06-29 | PARAMAGNETIC OXYGEN ANALYZER |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62327916A JPH0713626B2 (en) | 1987-12-24 | 1987-12-24 | Magnetic oximeter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01167653A JPH01167653A (en) | 1989-07-03 |
| JPH0713626B2 true JPH0713626B2 (en) | 1995-02-15 |
Family
ID=18204429
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62327916A Expired - Lifetime JPH0713626B2 (en) | 1987-06-29 | 1987-12-24 | Magnetic oximeter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0713626B2 (en) |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3302448A (en) | 1963-09-26 | 1967-02-07 | Honeywell Inc | Apparatus for supervising the proportion of a magnetically active component in a fluid |
| US3471776A (en) | 1968-01-09 | 1969-10-07 | Hays Corp | Fluid bridge method and means of detecting gases having magnetic susceptibility |
Family Cites Families (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4910280A (en) * | 1972-05-25 | 1974-01-29 | ||
| DE2522914C3 (en) * | 1975-05-23 | 1980-07-31 | Siemens Ag, 1000 Berlin Und 8000 Muenchen | Measuring device for determining the oxygen content in a gas mixture |
| JPS5312674A (en) * | 1976-07-22 | 1978-02-04 | Kishiyouchiyou Chiyoukan | Semiiconductor thermometer |
| JPH0681035B2 (en) * | 1984-12-19 | 1994-10-12 | 株式会社日立製作所 | Logic integrated circuit |
-
1987
- 1987-12-24 JP JP62327916A patent/JPH0713626B2/en not_active Expired - Lifetime
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3302448A (en) | 1963-09-26 | 1967-02-07 | Honeywell Inc | Apparatus for supervising the proportion of a magnetically active component in a fluid |
| US3471776A (en) | 1968-01-09 | 1969-10-07 | Hays Corp | Fluid bridge method and means of detecting gases having magnetic susceptibility |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH01167653A (en) | 1989-07-03 |
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