JPH01110232A - Viscosity vacuum gauge - Google Patents
Viscosity vacuum gaugeInfo
- Publication number
- JPH01110232A JPH01110232A JP26770887A JP26770887A JPH01110232A JP H01110232 A JPH01110232 A JP H01110232A JP 26770887 A JP26770887 A JP 26770887A JP 26770887 A JP26770887 A JP 26770887A JP H01110232 A JPH01110232 A JP H01110232A
- Authority
- JP
- Japan
- Prior art keywords
- disc
- gas
- rotational speed
- disk
- magnetic
- 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.)
- Pending
Links
Landscapes
- Measuring Fluid Pressure (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は低圧、希薄気体の圧力を測定する真空計に関
するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] This invention relates to a vacuum gauge for measuring the pressure of low pressure, dilute gas.
低圧、希薄な気体の圧力を測定する真空計として、従来
種々のものが実用化されているが、真空計の一種として
気体分子の平均自由行路が物体間の距離より大きい圧力
範囲では、運動する物体に働く気体の粘性力が圧力に比
例する性質を利用した粘性真空計がある。Various types of vacuum gauges have been put into practical use to measure the pressure of low-pressure, dilute gases. There is a viscous vacuum gauge that takes advantage of the property that the viscous force of gas acting on an object is proportional to pressure.
たとえば、平行な二つの円板の一方を回転さ七他方のね
じれを測定するラングミュアーダンシマンの分子真空計
や、細い水晶系を振動させてその減衰の速さから粘性力
を測定する管球などがある。Examples include Langmuir Dunciman's molecular vacuum gauge, which rotates one of two parallel disks and measures the torsion of the other, and a tube that vibrates a thin crystal system and measures viscous force from the rate of decay. and so on.
しかしながら従来のこうした粘性真空計では。 However, with conventional viscous vacuum gauges like this.
機械的摩擦や外部振動の影響や減衰の測定の困難さのた
めに、きわめて実用化がむつかしかった。It has been extremely difficult to put it into practical use due to the effects of mechanical friction and external vibration, and the difficulty in measuring damping.
この発明は上記のような問題点を解消するためになされ
たもので9機械的摩擦を−さい排除し。This invention was made to solve the above-mentioned problems by eliminating mechanical friction.
純粋に気体粘度の摩擦のみを容易な方法で測定できる装
置を得ることを目的としている。The purpose of this invention is to obtain a device that can measure purely gas viscosity friction in a simple manner.
この発明に係る粘性真空計は超電導物質でつくられた円
板を磁気浮上させ、さらにこの円板に非磁性体の円板と
羽根を付加して、これらを回転させた後、非接触で円板
の回転速度を測定するようKしたものである。The viscous vacuum gauge according to the present invention magnetically levitates a disc made of superconducting material, adds a non-magnetic disc and blades to this disc, rotates these, and then circles the disc in a non-contact manner. It is designed to measure the rotational speed of the plate.
この発明において、磁気浮上した超電導物質の円板およ
び非磁性体の円板と羽根は、気体との摩擦抵抗によって
のみ回転速度が減衰するので、この回転速度の減衰の度
合いを非接触で測定することにより、気体の粘度を求め
る。In this invention, since the rotational speed of the magnetically levitated superconducting disk and non-magnetic disk and blade is attenuated only by frictional resistance with the gas, the degree of attenuation of this rotational speed is measured without contact. By this, the viscosity of the gas is determined.
以下、この発明の一実施例を図について説明する。 An embodiment of the present invention will be described below with reference to the drawings.
図において、(1)は永久磁石、(2)は超電導物質で
つくられた円板、(3)は超電導物質の円板(2)に取
9つけられた非磁性体(たとえばプラスチックなど)の
円板、(4)は非磁性体の軸、(5)は非磁性体の羽根
。In the figure, (1) is a permanent magnet, (2) is a disk made of superconducting material, and (3) is a non-magnetic material (such as plastic) attached to disk (2) of superconducting material. A disc, (4) is a non-magnetic shaft, and (5) is a non-magnetic blade.
(6)は非磁性体の円板(3)の周辺にもうけられた穴
。(6) is a hole made around the non-magnetic disc (3).
(7)は発光装置、(8)は受光装置、(9)はパルス
カウンタである。(7) is a light emitting device, (8) is a light receiving device, and (9) is a pulse counter.
なお、超電導物質でつ(られた円板(2)と非磁性体の
円板(3)は中心位置を合わせて接合されてお飢さらに
軸(4)はこれら円板の中心に垂直に立てられている。The disk (2) made of superconducting material and the disk (3) made of non-magnetic material are joined with their centers aligned, and the axis (4) is erected perpendicularly to the center of these disks. It is being
超電導物質でつくられた円板(2)は、非磁性体でつ(
られた円板(3)、軸(4)9羽根(5)とともに、永
久磁石(1)のつ(る磁界によシ磁気浮上しており、他
のものとの機械的接触かまった(ない状態である。The disk (2) made of superconducting material is made of non-magnetic material (
The circular disk (3), shaft (4), and nine blades (5) are magnetically levitated by the magnetic field of the permanent magnet (1), and there is no mechanical contact with other objects. state.
この状態から、これら浮上している物体に、軸(4)を
中心としてコマをまわすように回転運動のみを与えると
、真空中では永久に回転しつづけるが。From this state, if only rotational motion is given to these floating objects, like spinning a top around the axis (4), they will continue to rotate forever in a vacuum.
気体中でこれを回転すると、気体との間の摩擦抵抗によ
多回転は徐々に減衰する。When it is rotated in gas, the rotation rate is gradually attenuated due to the frictional resistance between it and the gas.
この回転速度の減衰の度合いは、非磁性体の円板(3)
の周辺にもうけた穴(6)を通して発光装置(7)から
の光を受光装置(8)で受ければパルス状の信号が円板
の回転速度に比例して得られ、これをパルスカウンタ(
9)でカウントすることによシ、非接触状態で測定でき
るので9回転速度の減少が気体との摩擦抵抗のみによる
ものであることに変わシはない。The degree of attenuation of this rotational speed is determined by the non-magnetic disc (3).
When the light receiving device (8) receives the light from the light emitting device (7) through the hole (6) made around the disk, a pulse-like signal is obtained in proportion to the rotational speed of the disk, and this is sent to the pulse counter (
By counting at 9), measurement can be performed in a non-contact state, so there is no difference in the fact that the decrease in rotational speed is due only to the frictional resistance with the gas.
なお、上記実施例では気体との摩擦抵抗をより大きくし
て測定時間を短縮するために9羽根(5)ヲもうけであ
るが、必要に応じてその形状や羽根の枚数などを決めれ
ばよい。In the above embodiment, nine blades (5) are provided in order to increase the frictional resistance with the gas and shorten the measurement time, but the shape and number of blades may be determined as necessary.
また、軸(4)と羽根(5)がまったくないものでも。Also, even those without the shaft (4) and blades (5) at all.
円板と気体との間に摩擦抵抗は存在するので、測定の原
理は変わらない。Since frictional resistance exists between the disk and the gas, the principle of measurement remains the same.
なお1円板の回転速度の測定を非接触で行なうのに上記
実施例では2円板周辺に穴(6)ヲもうけたが2反射マ
ーカ等を円板表面に帖シ付けても非接触の測定は行なえ
る。In order to measure the rotational speed of the first disc without contact, in the above embodiment a hole (6) is provided around the second disc, but even if two reflective markers are attached to the surface of the disc, it is possible to measure the rotational speed of the second disc without contact. Measurements can be made.
磁気浮上させるための磁界を2本実施例では永久磁石か
ら得ているが、コイルを応用しても良い。In this embodiment, the magnetic field for magnetic levitation is obtained from two permanent magnets, but a coil may also be used.
以上のように、この発明によれば磁気浮上させた物体を
回転させてその回転速度の減衰を非接触で測定するよう
にしたので、水銀柱のようにこわれやすいものかまった
(な(堅牢で携帯に便利であり、経年変化部分かまった
(ないので定期的な校正を必要とせず、かつ構造が簡単
なため、きわめて安価な装置が得られる効果がある。As described above, according to this invention, a magnetically levitated object is rotated and the attenuation of its rotational speed is measured without contact. It is convenient, does not require periodic calibration because there are no parts that change over time, and has a simple structure, making it possible to obtain an extremely inexpensive device.
観構造図である。(1)は永久磁石、(2)は超電導物
質でつ(られた円板、(3)は非磁性体の円板、(4)
は非磁性体の軸、(5)は非磁性体の羽根、(6)は穴
、(7)は発光装置、(8)は受光装置、(9)はパル
スカウンタである。This is a perspective structural diagram. (1) is a permanent magnet, (2) is a disk made of superconducting material, (3) is a non-magnetic disk, (4)
is a non-magnetic shaft, (5) is a non-magnetic blade, (6) is a hole, (7) is a light emitting device, (8) is a light receiving device, and (9) is a pulse counter.
Claims (1)
成る羽根および円板を取りつけ気体中でこれらを回転さ
せた時の円板の回転速度を非接触で測定する機構をそな
えた粘性真空計。A viscous vacuum equipped with a disk made of a superconducting material, a blade made of a non-magnetic material, and a disk attached to the disk, and a mechanism for non-contact measurement of the rotational speed of the disk when it is rotated in a gas. Total.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP26770887A JPH01110232A (en) | 1987-10-23 | 1987-10-23 | Viscosity vacuum gauge |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP26770887A JPH01110232A (en) | 1987-10-23 | 1987-10-23 | Viscosity vacuum gauge |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH01110232A true JPH01110232A (en) | 1989-04-26 |
Family
ID=17448442
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP26770887A Pending JPH01110232A (en) | 1987-10-23 | 1987-10-23 | Viscosity vacuum gauge |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH01110232A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH06288854A (en) * | 1993-03-31 | 1994-10-18 | Agency Of Ind Science & Technol | Rotary viscosity vacuum gauge |
| JPH09292300A (en) * | 1996-04-26 | 1997-11-11 | Agency Of Ind Science & Technol | Rotary type viscosity vacuum gauge |
| JP2005331362A (en) * | 2004-05-20 | 2005-12-02 | Canon Inc | Vacuum gauge |
-
1987
- 1987-10-23 JP JP26770887A patent/JPH01110232A/en active Pending
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH06288854A (en) * | 1993-03-31 | 1994-10-18 | Agency Of Ind Science & Technol | Rotary viscosity vacuum gauge |
| JPH09292300A (en) * | 1996-04-26 | 1997-11-11 | Agency Of Ind Science & Technol | Rotary type viscosity vacuum gauge |
| JP2005331362A (en) * | 2004-05-20 | 2005-12-02 | Canon Inc | Vacuum gauge |
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