JPS58169044A - Constant temperature type pirani vacuum gauge - Google Patents

Constant temperature type pirani vacuum gauge

Info

Publication number
JPS58169044A
JPS58169044A JP57052557A JP5255782A JPS58169044A JP S58169044 A JPS58169044 A JP S58169044A JP 57052557 A JP57052557 A JP 57052557A JP 5255782 A JP5255782 A JP 5255782A JP S58169044 A JPS58169044 A JP S58169044A
Authority
JP
Japan
Prior art keywords
circuit
vacuum
output
resistor
gauging
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.)
Granted
Application number
JP57052557A
Other languages
Japanese (ja)
Other versions
JPH029294B2 (en
Inventor
Noboru Kuriyama
昇 栗山
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.)
Tokuda Seisakusho Co Ltd
Original Assignee
Tokuda Seisakusho Co Ltd
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 Tokuda Seisakusho Co Ltd filed Critical Tokuda Seisakusho Co Ltd
Priority to JP57052557A priority Critical patent/JPS58169044A/en
Publication of JPS58169044A publication Critical patent/JPS58169044A/en
Publication of JPH029294B2 publication Critical patent/JPH029294B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L21/00Vacuum gauges
    • G01L21/10Vacuum gauges by measuring variations in the heat conductivity of the medium, the pressure of which is to be measured
    • G01L21/12Vacuum gauges by measuring variations in the heat conductivity of the medium, the pressure of which is to be measured measuring changes in electric resistance of measuring members, e.g. of filaments; Vacuum gauges of the Pirani type

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Volume Flow (AREA)
  • Measuring Fluid Pressure (AREA)

Abstract

PURPOSE:To indicate atmospheric pressure in inverse proportion when a Pirani gauging resistance etc. is abnormal, by a method wherein a bridge circuit comprising a Pirani gauging resistance is combined with an offset amplifier and a feedback circuit with a by-pass feeder. CONSTITUTION:Heat release from a Pirani gauging resistance Rs depends on atmosphere to be measured. It is less in low pressure, and increases as atmosphere to be measured approaches to atmospheric pressure. Voltage VE corresponding to heat release electric power Ps is max. in atmospheric pressure, and is min. in vacuum, while a gauging output Vout is 0V in atmospheric pressure, and is full-scale in vacuum as it is an inverse output of VE. When some abnormality occurs in the circuit, or the Pirani gauging resistance Rs is short-circuitted or disconnected, the gauging output Vout is shown as 0V. Further, the resistance Rs is opened, the gauging output Vout is also shown as 0V.

Description

【発明の詳細な説明】 本発明は真空計に係り1%に定温度形ビラニー真空針に
関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a vacuum gauge, and relates to a constant temperature Villany vacuum needle.

この糧真空針は金属油線状のビラニー測定抵抗(これを
R8と呼ぶ)を3つの抵抗←R1* R1*Rs  )
と組合わせてブリダシ回路を構成し、このブリ、ジ回路
に給電してR8の温度を一定に保とうとするとき 真空
度いかんくよるR8の放熱量変化に応じてブリ、ジ園路
うの供給電流が変化することで真空度を測定する本ので
ある。この供給電流の増減によりR6の温度したがって
抵抗値が一定に保たれるところから定温度形と呼ばれる
This food vacuum needle has three resistances (R1*R1*Rs) with a metal oil line-shaped Villany measuring resistance (this is called R8).
When trying to keep the temperature of R8 constant by supplying power to this circuit, the power supply is supplied in response to the change in the amount of heat dissipated from R8 depending on the degree of vacuum. This is a book that measures the degree of vacuum by changing the current. It is called a constant temperature type because the temperature and therefore the resistance value of R6 are kept constant by increasing or decreasing the supplied current.

従来このような回路はウィーンブリ、ジ発振回路に組込
まれていて振幅を決めるG11l!素としてR8が用い
られている。
Conventionally, such a circuit has been incorporated into a WienBrie oscillation circuit, and G11l! which determines the amplitude. R8 is used as the element.

しかしながら、この真空計は温度特性が悪いとか発振回
路に用いられる増幅器の利得による影響を受けるとかの
不具合がある上に、測定値の指示方法が異常発生時に真
空状態と同じ指示を行う点で重大な不都合がちす、この
異常時に低気圧として指示するということは、真空計の
出力に基き真空装置の動作制御を行う場合に不都合な事
態が生じることになる。たとえばビラニー測定抵抗の電
源が切れた場合に低気圧の指示が行われると、真空装蓋
は処理動作を継続してよいことKなり、動作シーケンス
はそのtt続行される。これは真空度を測定せずに処理
動作を行っていることに等しいから不都合な事態を生じ
ることになる。
However, this vacuum gauge has problems such as poor temperature characteristics and is affected by the gain of the amplifier used in the oscillation circuit, and is also important in that the method of indicating the measured value is the same as in a vacuum state when an abnormality occurs. Inconveniently, instructing as low pressure at the time of this abnormality causes an inconvenient situation when controlling the operation of the vacuum device based on the output of the vacuum gauge. For example, if the Villany measuring resistor is de-energized and a low pressure indication is given, the vacuum cover may continue processing operations and the operating sequence continues. This is equivalent to performing a processing operation without measuring the degree of vacuum, resulting in an inconvenient situation.

本発明は上述の点に鑑みてなされたもので、ビラニー測
定抵抗による真空度測定信号を極性反転させた上で取出
すようKすると共に、ビラニー測定抵抗が短絡状聰にな
っても開放状態になっても大気圧状態の指示を行う定温
度形ビラニー真空針を構成したものである。
The present invention has been made in view of the above-mentioned points, and is capable of reversing the polarity of the vacuum degree measurement signal from the Villany measuring resistor before taking it out, and also ensuring that even if the Villany measuring resistor becomes short-circuited, it will be in an open state. It consists of a constant temperature Villany vacuum needle that indicates the atmospheric pressure state even when the pressure is on.

以下添付図面を参照して本発明の一実施例を説明する。An embodiment of the present invention will be described below with reference to the accompanying drawings.

図においてR,はビラニー測定抵抗でるに、抵抗R1+
 R1e R1と共にプリジ回路を構成してお抄、ビラ
ニー測定抵抗R8はケーブルおよびノイズフィルタIP
を介してブリ、ジ回路の他の抵抗に接続されている。こ
のブリ、ジ回路にはフィードバック回路FBから抵抗R
・を介して給電され、その出力点ム、Bの出力はそれぞ
れ抵抗R4。
In the figure, R is the Villany measurement resistance, and the resistance R1+
R1e R1 together with R1 constitutes a circuit, and Villany measurement resistor R8 is connected to the cable and noise filter IP.
is connected to other resistors in the circuit via This bridge circuit is connected to a resistor R from the feedback circuit FB.
・The outputs of the output points M and B are each connected to a resistor R4.

R,を介して増幅器工01に与えられる。ここで、抵抗
R4+ ”lを適当に選択して増幅器101の入力バイ
アス電流によりオフセットをかけ、低気圧測定時に起き
得る発振を防止する。”4  e R1の@保は増幅器
工01のバイアス電流が流れ出すときはR4<< Rm
、流れ込むときはR4>>R1とする。この増幅器工O
1の出力端哄抵抗R@+R?を介して電源+端子に接続
されており、抵抗R・とR7との相互接続点が逆流阻止
ダイオードDIを介してフィードパ、り回路?Bのトラ
ンジスタQのペースに接続されている。トランジスタQ
のコレクタ・エミ、り関にはバイパス抵抗RBが並ぢ 列接続されており、その工ξ、タ出力を前述の如く抵抗
Roを介してブリ、ジ回路に与えると共K、抵抗R―を
介して極性反転増幅器工0雪の反転入力端に与える。こ
の増幅器工03は反転入力端が抵抗R,を介して抵抗R
111および可変抵抗VRからなる可変電圧源に接続さ
れてお抄、一方非反転入力端は抵抗Ituを介して接地
されている。そして増幅器工0雪の入出力端間には、抵
抗R1t、コンデンサO,およびダイオードp3の並列
回路に抵抗Rtsを直列接続してなるフィードパ、り要
素が接続されており、並列回路と抵抗R1mとの相互接
続点から測定出力を取出すようになっている。
R, to the amplifier engineer 01. Here, the resistor R4 + ``1'' is appropriately selected to apply an offset with the input bias current of the amplifier 101 to prevent oscillations that may occur during low pressure measurement. When it begins to flow, R4<< Rm
, when flowing, R4>>R1. This amplifier engineer
1 output terminal resistance R@+R? The interconnection point between resistors R and R7 is connected to the power supply + terminal through a reverse current blocking diode DI, and the feed circuit is connected to the power supply + terminal via It is connected to the pace of transistor Q of B. transistor Q
A bypass resistor RB is connected in parallel to the collector emitter and resistor of the circuit, and when the output of the resistor RB is applied to the circuit through the resistor Ro as described above, the resistor K and the resistor R- are connected in parallel. It is applied to the inverting input terminal of the polarity inverting amplifier through the inverting input terminal. In this amplifier 03, the inverting input terminal is connected to the resistor R through the resistor R.
111 and a variable voltage source consisting of a variable resistor VR, while the non-inverting input terminal is grounded via a resistor Itu. Between the input and output terminals of the amplifier is connected a feed pad element consisting of a parallel circuit of a resistor R1t, a capacitor O, and a diode p3 with a resistor Rts connected in series, and a parallel circuit and a resistor R1m. The measurement output is taken out from the interconnection point.

仁の回路の動作は次の通りである。The operation of Jin's circuit is as follows.

ビラニー測定抵抗R8は被測定雰囲気に応じて放熱する
もので放熱量は低気圧つtb高真空早は少く、大気圧に
近づくKつれて放熱量が増す。放熱量は電力P8で表わ
すと。
The Villany measurement resistor R8 radiates heat depending on the atmosphere to be measured, and the amount of heat radiated is small at low pressure and high vacuum, and increases as the pressure approaches atmospheric pressure. The amount of heat radiation is expressed as electric power P8.

P ロX  R8 であり、ブリリジが平衡したときのFランジスタQの工
ξ、タ電圧Vヨは。
P roX R8 , and when the bridge is balanced, the power ξ and the voltage V yo of the F transistor Q are.

v、−xFtl   1c:比例定数 とな抄、放熱電力P8に対応した電圧vRが得られる。v, -xFtl 1c: Constant of proportionality A voltage vR corresponding to the heat dissipation power P8 is obtained.

そして、この電圧V、け被測定雰囲気が大気圧で最大、
真空で最小となるが、測定出力Voutはその反転され
たものであるから大気圧でOv。
This voltage V is the maximum when the atmosphere to be measured is atmospheric pressure,
It is minimum in vacuum, but the measured output Vout is the inverse of that, so it is Ov at atmospheric pressure.

真空でフルスケールとなる。Full scale in vacuum.

この測定出力Tautの値は、電圧V、により抵抗R1
に流れる電流工、魯と可変電圧源電圧v8により抵抗R
書に流れる電流IPとの和の電流が74−ドパツク豐素
中の抵抗R1mを流れるので。
The value of this measurement output Tout is determined by the voltage V and the resistance R1
The current flowing through the resistor R due to the current flow and the variable voltage source voltage v8
Since the sum of the current IP and the current flowing through the resistor R1m in the 74-doped silicon element flows through the resistor R1m.

Vout−−RHg (IRI十工R―)となる。そこ
で、IR@を として、R13の値を適当に選べば大気圧でVOut−
O1真空で所定値たとえば10Vとすることができる。
Vout--RHg (IRI Juuko R-). Therefore, if we take IR@ and choose the value of R13 appropriately, VOut-
A predetermined value, for example 10V, can be set at O1 vacuum.

次に回路上の異常が発生した場合の動作を述べる。回路
上の異常としては主としてビラニー測定抵抗R8の短絡
または断線があげられる。この抵抗R8は極く細い線を
被測定雰囲気中に露出させて使用するものだからである
Next, the operation when a circuit abnormality occurs will be described. The circuit abnormality mainly includes a short circuit or disconnection of the Villany measuring resistor R8. This is because this resistor R8 is used by exposing an extremely thin wire to the atmosphere to be measured.

まず抵抗RBが短絡した場合、ブリッジ回路のム点の電
圧がOであるからv、Fi最大値、したがって測定出力
Vout−07となる。ダイオードD3はこのときの出
力が−になり過ぎないようにクランプするために設けら
れている。
First, when the resistor RB is short-circuited, since the voltage at the point M of the bridge circuit is O, the maximum value of v and Fi, and hence the measured output Vout-07. The diode D3 is provided to clamp the output at this time so that it does not become too negative.

また抵抗R8が開放の場合、ブリ、ジ回路のム点の電圧
〉B点の電圧でトランジスタqがオフになる。この場合
、プリ雫ジ回路への給電は抵抗RB、R・を介して行わ
れる。ここで抵抗RBの抵抗値はブリ、ジ回路の抵抗R
*  + ”*のそれより捕かに小さく選んであるから
電圧vBFi鏝大値で測定出力VoutがOVとなる。
Further, when the resistor R8 is open, the transistor q is turned off when the voltage at the point M>the voltage at the point B of the bridge circuit. In this case, power is supplied to the pre-drop circuit via resistors RB and R. Here, the resistance value of resistor RB is the resistance R of the circuit.
Since it is selected to be considerably smaller than that of * + "*, the measured output Vout becomes OV at the maximum value of the voltage vBFi.

すなわちピラニー測定抵抗R8が短絡または断線すると
測定出力VOutは大気圧測定時と同じくOVとなる。
That is, if the Pirani measurement resistor R8 is short-circuited or disconnected, the measurement output VOut becomes OV, the same as when measuring atmospheric pressure.

これは測定出力Voutで真空機器を動作制御する場合
、動作シーケンスを停止させ得ることを意味している。
This means that when controlling the operation of vacuum equipment using the measurement output Vout, the operation sequence can be stopped.

本発明は上述のように、ビラニー測定抵抗を含むブリ、
ジ回路を、オフセットをかけた増幅器およびバイパス給
電路付きのフィードパ、り回路と組合わせることKよや
気圧に比例関係の測定信号を得、これを俸性反転回路を
介して出力するようにした丸め、気圧と逆比例関係でし
かもビラニー測定抵抗や電源勢に異常があるとき大気圧
の指示を行う真空計を提供することができる。
As described above, the present invention includes a bridge including a Villany measuring resistor,
By combining the circuit with a feed circuit with an offset amplifier and a bypass feed path, a measurement signal proportional to the atmospheric pressure was obtained, and this was output via a salary inversion circuit. It is possible to provide a vacuum gauge that is inversely proportional to atmospheric pressure and that indicates atmospheric pressure when there is an abnormality in the Villany measurement resistance or power supply.

また、本発明#′i厘流側流動作形るところから同一1
−流電源に複数の回路を接続することにより。
In addition, the present invention #'i has the same flow side flow operation form.
– by connecting multiple circuits to a current source.

相−4干渉を生ぜずに多点を同時測定することができ、
しかも制御用の圧力測定回路としてコンパクトに構成で
きる。
Multiple points can be measured simultaneously without phase-4 interference,
Moreover, it can be configured compactly as a pressure measurement circuit for control.

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

図は本発明の一実施例の回路図である。 R8・・・ピラニー測定抵抗、RB・・・バイパス抵抗
、R1〜R11”’抵抗、VR−・・可変抵抗、 I 
ol、IOs・・・増幅器、Q・・・トランジスタ、D
I  ! DI・・・ダイオード、MP・・・ノイズフ
ィルタ、IFB・・・フィードバック回路。 出願人代理人  猪  股     清手続補正書 1.・j[件の表示 昭和57年特許願第52557号 2、発明の名称 定温度形ビラニー真空計 3、補正をする者 事件との関係特許出願人 7、補正の対象 明細書の全文および図面
The figure is a circuit diagram of an embodiment of the present invention. R8...Pirani measurement resistance, RB...Bypass resistance, R1~R11"' resistance, VR-...Variable resistance, I
ol, IOs...amplifier, Q...transistor, D
I! DI...diode, MP...noise filter, IFB...feedback circuit. Applicant's agent Kiyoshi Inomata Procedural amendment 1.・J [Indication of 1982 Patent Application No. 52557 2, Name of the invention Constant temperature Villany vacuum gauge 3, Person making the amendment Relationship to the case Patent applicant 7, Full text of the specification subject to the amendment and drawings

Claims (1)

【特許請求の範囲】 1、ビラニー測定抵抗および固定抵抗により構成され真
空測定時に小出力で大気圧測定時に大出力を生じるブリ
、ジ回路と、このブリ、ジ回路の出力を増幅する増幅器
と、この増幅器の出力に応じ前記ブリ、ジ回路に給電す
るフィードパ、り回路と、このフィードパ、り回路に並
列接続されて前記ブリ、ジ回路に給電するパイ鍾ス抵抗
と、前記増幅器の出力を極性反転して出力する回路とを
そなえ九定温度形ピラニー真空針。 コ41許請求の範囲第7項記載の真空計において。 紬配増幅器の入力端子にオフセットをかけてなる定温度
形ピラニー真空針。 7.411許晴求の範囲第1項または第2項記載の真空
計において、前記ビラニー測定抵抗をノイズフィルタを
介して酌配ブリ、ジ回路に接続してなる定温度形ビラニ
ー真空針。
[Scope of Claims] 1. A BRI circuit that is composed of a Villany measuring resistor and a fixed resistor and produces a small output when measuring vacuum and a large output when measuring atmospheric pressure, and an amplifier that amplifies the output of this BRI circuit; A feed path circuit that supplies power to the bridge circuit according to the output of the amplifier, a bias resistor that is connected in parallel to the feed path circuit and feeds power to the bridge circuit, and a polarity polarity for the output of the amplifier. Nine constant temperature type Pirani vacuum needles equipped with an inverted output circuit. 41. In the vacuum gauge according to claim 7. A constant temperature Pirani vacuum needle that applies an offset to the input terminal of a Tsumugi amplifier. 7.411 Range of Permissible Requests A constant temperature type Villany vacuum needle in the vacuum gauge according to item 1 or 2, wherein the Villany measuring resistor is connected to a power distribution circuit through a noise filter.
JP57052557A 1982-03-31 1982-03-31 Constant temperature type pirani vacuum gauge Granted JPS58169044A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57052557A JPS58169044A (en) 1982-03-31 1982-03-31 Constant temperature type pirani vacuum gauge

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57052557A JPS58169044A (en) 1982-03-31 1982-03-31 Constant temperature type pirani vacuum gauge

Publications (2)

Publication Number Publication Date
JPS58169044A true JPS58169044A (en) 1983-10-05
JPH029294B2 JPH029294B2 (en) 1990-03-01

Family

ID=12918111

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57052557A Granted JPS58169044A (en) 1982-03-31 1982-03-31 Constant temperature type pirani vacuum gauge

Country Status (1)

Country Link
JP (1) JPS58169044A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01154441U (en) * 1988-04-18 1989-10-24
JPH0430056U (en) * 1990-06-29 1992-03-11
JP2009062096A (en) * 2008-12-24 2009-03-26 Nitto Pack Kk Bag-like easy opening package

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01154441U (en) * 1988-04-18 1989-10-24
JPH0430056U (en) * 1990-06-29 1992-03-11
JP2009062096A (en) * 2008-12-24 2009-03-26 Nitto Pack Kk Bag-like easy opening package

Also Published As

Publication number Publication date
JPH029294B2 (en) 1990-03-01

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