JPS6066362A - Sealing device - Google Patents

Sealing device

Info

Publication number
JPS6066362A
JPS6066362A JP58175040A JP17504083A JPS6066362A JP S6066362 A JPS6066362 A JP S6066362A JP 58175040 A JP58175040 A JP 58175040A JP 17504083 A JP17504083 A JP 17504083A JP S6066362 A JPS6066362 A JP S6066362A
Authority
JP
Japan
Prior art keywords
magnetic
temperature
magnetic fluid
sealing device
permanent magnet
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
JP58175040A
Other languages
Japanese (ja)
Other versions
JPH0363149B2 (en
Inventor
Hiroshi Nakazato
博 中里
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.)
Tokin Corp
Original Assignee
Tohoku Metal Industries 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 Tohoku Metal Industries Ltd filed Critical Tohoku Metal Industries Ltd
Priority to JP58175040A priority Critical patent/JPS6066362A/en
Publication of JPS6066362A publication Critical patent/JPS6066362A/en
Publication of JPH0363149B2 publication Critical patent/JPH0363149B2/ja
Granted legal-status Critical Current

Links

Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F16ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
    • F16JPISTONS; CYLINDERS; SEALINGS
    • F16J15/00Sealings
    • F16J15/16Sealings between relatively-moving surfaces
    • F16J15/40Sealings between relatively-moving surfaces by means of fluid
    • F16J15/43Sealings between relatively-moving surfaces by means of fluid kept in sealing position by magnetic force

Landscapes

  • Engineering & Computer Science (AREA)
  • General Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Sealing Using Fluids, Sealing Without Contact, And Removal Of Oil (AREA)
  • Rotational Drive Of Disk (AREA)

Abstract

PURPOSE:To keep the pressure resistance inside a sealing device constant even if the environmental temperature is changed by constituting a portion on the way of a magnetic path or a portion adjacent to the magnetic path of a heat sensitive magnetic body. CONSTITUTION:As shown in the sectional view, a sealing device is constituted of pole pieces 2 contacted both sides of a ring-like permanent magnet 1, magnetic rotary body 4 and magnetic fluid 3 caught between the pole pieces 2 and the rotary body 4. A annular temperature sensitive magnetic fluid 5 is interposed between the right and left pole pieces 2 so as to touch the inner periphery of the permanent magnet 1. For instance, Mn-Zn group heat sensitive ferrite or the like is used as the heat sensitive magnetic body.

Description

【発明の詳細な説明】 本発明はコンピュータ用磁気ディスクのダストシール装
置、真空装置の回転軸シール装置及び空気弁等に適用し
て好適な磁性流体を利用I−だ密封装置だ関するもので
ある。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an I-type sealing device using a magnetic fluid suitable for application to a dust sealing device for a magnetic disk for a computer, a rotary shaft sealing device for a vacuum device, an air valve, and the like.

例えば磁気ディスク装置においては、外部に設置したモ
ータから延長形成した回転軸の端部に、ディスク部を取
り付けることがあり、このディスク設置両所と外部とは
ディスク部への塵埃又はベアリング等から発生するオイ
ルミスト等の侵入を防ぐため、空気流通を遮断する密封
装置が設けられることかある。
For example, in a magnetic disk drive, the disk unit is sometimes attached to the end of a rotating shaft extended from a motor installed externally, and dust on the disk unit or from bearings, etc. In order to prevent the intrusion of oil mist, etc., a sealing device that blocks air circulation is sometimes provided.

第1図は一般的なこの種密@装置の一例を示す断面図で
ある、環状の永久磁石1の両側iで環状強磁性体(ポー
ルピース)2が取り付けられ、強磁性回転体4が環状体
2に挿入され、ポールピース2と回転軸4との間l(形
成された環状空隙に、磁性流体3が磁気的に捕捉されて
いる。該磁性流体3のこの環状膜により密封装置として
機能している。
FIG. 1 is a cross-sectional view showing an example of a general type device. An annular ferromagnetic body (pole piece) 2 is attached to both sides i of an annular permanent magnet 1, and a ferromagnetic rotating body 4 is attached to the annular permanent magnet 1. The magnetic fluid 3 is magnetically captured in the annular gap formed between the pole piece 2 and the rotating shaft 4. This annular film of the magnetic fluid 3 functions as a sealing device. are doing.

ところで、磁性流体が形成する環状膜は、所定量の磁性
流体をポールピース2と回転軸4との間1(注入しなけ
れば密封装置としての耐圧が充分に発生せず、密封装置
として機能を果たさないことは周知である。しかし、充
分な量の磁性流体を注入し、放置状態又は動作時におい
て、磁性流体3が環境温度の上昇により密封装置の外部
へ流出して密封空間を汚染する欠点がある。その原因は
第1に、2つの環状磁性流体で仕切られた空間にある空
気が熱膨張して、環状磁性流体膜3を密封装置外部へ押
圧する。第2に、環境温度の上昇により永久磁石1の供
給できる磁束量が低減する。従って、磁性流体膜3を保
持固定する磁界の減少によりシール耐圧が低下し、第1
の理由に掲げた力により磁性流体膜3が移動し易くなる
か、磁性流体膜3が破れて、磁性流体か4密封装置の外
部へ流出する。第3図(で、環境温度の上昇により、磁
性流体自体からの飽和磁化が低減し、よってシール耐圧
が減少する。その結果前述の力により、磁性流体膜3が
移動1−易くなるか、磁性流体膜3が破れて磁性流体が
密封装置産外部へ流出する。第4に、環境温度が上昇す
ると磁性流体の表面張力及び粘度が低下して(る。従っ
て、磁性流体膜3が前述の力により移動し易くなる。こ
れらの原因が考えられる。
By the way, the annular film formed by the magnetic fluid is such that if a predetermined amount of magnetic fluid is not injected between the pole piece 2 and the rotating shaft 4 (1), sufficient withstand pressure will not be generated as a sealing device, and it will not function as a sealing device. However, when a sufficient amount of magnetic fluid is injected and the magnetic fluid 3 is left unused or in operation, the magnetic fluid 3 flows out of the sealed device due to an increase in environmental temperature and contaminates the sealed space. The first reason is that the air in the space partitioned by the two annular magnetic fluids expands thermally and presses the annular magnetic fluid film 3 to the outside of the sealing device.Second, the environmental temperature increases. As a result, the amount of magnetic flux that can be supplied by the permanent magnet 1 is reduced.Therefore, due to the decrease in the magnetic field that holds and fixes the magnetic fluid film 3, the sealing pressure is reduced, and the first
Due to the force mentioned in the above reason, the magnetic fluid film 3 becomes easy to move or the magnetic fluid film 3 is torn, and the magnetic fluid flows out of the sealing device. As the environmental temperature increases, the saturation magnetization from the magnetic fluid itself decreases, and the sealing pressure decreases.As a result, due to the aforementioned force, the magnetic fluid film 3 becomes easier to move, or the magnetic fluid film 3 becomes easier to move. The fluid film 3 is ruptured and the magnetic fluid flows out of the sealed device.Fourth, as the environmental temperature rises, the surface tension and viscosity of the magnetic fluid decrease. This makes it easier to move.These are possible causes.

ところで、磁性流木による密封機構を有する左右の空間
は流体の遮1所がなされているが、例えば空気弁等のよ
うにある温度領域では流体の流通を促進したり逆((遮
断する必要がある。しかし、従来のこの種密封機構は上
述したような欠点があり、作為的に磁性流体のパルプ(
弁)作用を行なわせることは至難である。
By the way, the left and right spaces that have a sealing mechanism using magnetic driftwood are blocked from fluid at one point, but in a certain temperature range, for example, air valves, etc., can promote the flow of fluid or vice versa ((it is necessary to block it). However, this type of conventional sealing mechanism has the above-mentioned drawbacks, and the magnetic fluid pulp (
It is extremely difficult to make the valve work.

本発明はかかる点に鑑み、対境温度の上昇に伴う密封機
能の低下を抑制するため、磁路中に感温磁性体を設げ、
感温磁性体の任意の設定により所定の温度領域で密封機
溝の増加又は減少を作為的に行ない得る密封装置を提案
することを主たる目的とする。
In view of this point, the present invention provides a temperature-sensitive magnetic material in the magnetic path in order to suppress the deterioration of the sealing function due to the rise in the ambient temperature,
The main purpose of the present invention is to propose a sealing device that can intentionally increase or decrease the sealing groove in a predetermined temperature range by arbitrarily setting the temperature-sensitive magnetic material.

以下本発明の一実施例について図面を参照しながら詳粗
に説明する。
An embodiment of the present invention will be described in detail below with reference to the drawings.

第2図は本発明の一例を示す断面図である。環状の永久
磁石1、この両側IC接したポールピース2、磁性回転
体4及びボ・−ルピース2と回転体4との間に捕捉され
た磁性流体13による密封装置(以下MFSという)が
構成されていることは従来通りであるが、更に永久磁石
1の内周面に接して環状の感温磁性流体5が左右のポー
ルピース2に挾持されている。感温磁性材5は例えばM
n −Zn系感温フェライトを用い得る。
FIG. 2 is a sectional view showing an example of the present invention. A sealing device (hereinafter referred to as MFS) is composed of an annular permanent magnet 1, a pole piece 2 in contact with the IC on both sides, a magnetic rotating body 4, and a magnetic fluid 13 trapped between the ball piece 2 and the rotating body 4. However, an annular temperature-sensitive magnetic fluid 5 is sandwiched between the left and right pole pieces 2 in contact with the inner peripheral surface of the permanent magnet 1. The temperature-sensitive magnetic material 5 is, for example, M
An n-Zn temperature-sensitive ferrite can be used.

第3図は、温度変化とMFS耐圧との関係を示す線図で
ある。感温磁性体5のキュリ一点(Tc)以下の温度領
域では、永久磁石1からの磁束力?ポールピース2を通
過して強磁性回転体4へ作用せず、ポールピース2から
感温磁性体5を通過し、他方のポールピース2を経て永
久磁石1へ戻って(るので、M FSの耐圧は殆んど発
生しない。キュリ一点Tc付近の温度から上昇すると、
感温フェライトの飽和磁化が減少し始めるから、感温フ
ェライト5を通過1−る磁束量が減少し、磁束は逆にポ
ールピース2かも磁性流体3を通過し、回転軸4を通過
する。磁束量の増加に伴ないMFSの耐圧が増大してく
る(第3図中曲線B診照)。従って、感温フェライト5
0作用による回転体4に作用づ−る磁束量が温度上昇と
共に増大するキュリ一点以上の温度頒或では、ポールピ
ース2、磁性流体膜3及び回転軸4に作用する磁束の増
加と磁性流体3の飽和磁化の減少量とが平衡して、MF
Sの耐圧が一定となる。それ以上の高温領域では、第3
図に示す如(、永久磁石が供給する磁性流体3を通過保
持する磁束密度も減少し、磁性流体の飽和磁化も減少す
るので、MFSの耐圧は徐々に減少する。
FIG. 3 is a diagram showing the relationship between temperature change and MFS breakdown voltage. In the temperature range below the Curie point (Tc) of the temperature-sensitive magnetic material 5, the magnetic flux force from the permanent magnet 1? The MFS does not pass through the pole piece 2 and act on the ferromagnetic rotating body 4, but passes from the pole piece 2 through the temperature-sensitive magnetic body 5, passes through the other pole piece 2, and returns to the permanent magnet 1. Almost no breakdown voltage occurs.When the temperature rises from around the Curie point Tc,
Since the saturation magnetization of the temperature-sensitive ferrite begins to decrease, the amount of magnetic flux passing through the temperature-sensitive ferrite 5 decreases, and conversely, the magnetic flux also passes through the pole piece 2, the magnetic fluid 3, and the rotating shaft 4. As the amount of magnetic flux increases, the withstand voltage of the MFS increases (see curve B in FIG. 3). Therefore, temperature-sensitive ferrite 5
At temperature distribution above the Curie point, where the amount of magnetic flux acting on the rotating body 4 due to the zero effect increases with temperature rise, the magnetic flux acting on the pole piece 2, the magnetic fluid film 3, and the rotating shaft 4 increases and the magnetic fluid 3 increases. In equilibrium with the amount of decrease in saturation magnetization of MF
The withstand voltage of S becomes constant. In higher temperature ranges, the third
As shown in the figure, the magnetic flux density that passes through and holds the magnetic fluid 3 supplied by the permanent magnet decreases, and the saturation magnetization of the magnetic fluid also decreases, so the withstand voltage of the MFS gradually decreases.

従って、MFSの耐圧一定の温度領域をM F S動作
環境の変動域に設定することにより、Ml”Sの温度−
F昇如よる耐圧低下を補償して磁性流体3の流出を防止
できる。
Therefore, by setting the temperature range where the MFS's withstand voltage is constant to the variable range of the MFS operating environment, the temperature of Ml''S -
The leakage of the magnetic fluid 3 can be prevented by compensating for the drop in withstand pressure due to the increase in F.

更処、感温フェライト5の断面積や材質、永久磁石1の
断面積や材質等を考慮することによって、第3図中曲線
Cの如く、温度上昇に伴ってMPSの耐圧を徐々に増加
せ1−め得る。また磁性流体3固有の表面張力及び粘度
低下による磁性流体3の流出も、みかけの磁性流体の粘
度増加現象(磁性流体に印加される磁界強度を増加する
と、それ(て伴って磁性流体の粘度が増加する現象)に
より、防止することができる。尚、第3図中、曲線Aは
第1図例の構造による変化を参考に示しているが、温度
上昇に伴い、耐圧特性が悪化していることが理解される
。その理由は前述した通りである。
By considering the cross-sectional area and material of the temperature-sensitive ferrite 5, the cross-sectional area and material of the permanent magnet 1, etc., the withstand voltage of the MPS can be gradually increased as the temperature rises, as shown by curve C in Fig. 3. I can get 1st. In addition, the outflow of the magnetic fluid 3 due to the surface tension and viscosity reduction inherent to the magnetic fluid 3 is also caused by the phenomenon of an apparent increase in the viscosity of the magnetic fluid (as the magnetic field strength applied to the magnetic fluid increases, the viscosity of the magnetic fluid 3 increases). Curve A in Figure 3 shows the change due to the structure of the example in Figure 1 as a reference, but as the temperature rises, the withstand voltage characteristics deteriorate. It is understood that the reason is as mentioned above.

第4図は磁束のバイパスとI−て用いた感温フェライト
5を、永久磁石1、ポールピース2の外側に配置した他
の実施例である。動作原理及び効果は図2の実施例と同
じであるので、詳細説明を省(・ 次に、MFSの耐圧の温度依存性を自由に形成すること
がriT能な本発明の実施例(7I:つ(・て以下して
説明する。
FIG. 4 shows another embodiment in which a temperature-sensitive ferrite 5 used as a magnetic flux bypass and an I- is arranged outside the permanent magnet 1 and the pole piece 2. Since the operating principle and effects are the same as those of the embodiment shown in FIG. 2, a detailed explanation will be omitted. This will be explained below.

第5図は、感温フェライト5と永久磁石1とをポールピ
ース2でザノドウイソチ状に挾んだ構造を有するMFS
の一例を示す断面図である。感温フェライト5のギコー
リ一点Tc以下の温度では、永久磁石1の有する起磁力
はポールピース2と回転体4との空隙仄のみ費されるの
で、第6図に示す如く、M、FSとしての耐圧は太きい
。しかし温度」1昇により、Tc付近から感温フェライ
ト5の飽和磁化が急激に低下する段になると、それ(/
′C従って、感温フェライト5の起磁力損失が増大し、
MFSの耐圧が急激に減少するようになる。従って、こ
のような特性を利用して磁性流体による隔壁の温度変化
による開閉を行ブよ5ことができる。
Figure 5 shows an MFS having a structure in which a temperature-sensitive ferrite 5 and a permanent magnet 1 are sandwiched between pole pieces 2 in a diagonal shape.
It is a sectional view showing an example. At a temperature below the Gikori point Tc of the temperature-sensitive ferrite 5, the magnetomotive force of the permanent magnet 1 is used only in the gap between the pole piece 2 and the rotating body 4, so as shown in FIG. High pressure resistance. However, when the temperature rises by 1, the saturation magnetization of the temperature-sensitive ferrite 5 rapidly decreases from around Tc,
'C Therefore, the magnetomotive force loss of the temperature-sensitive ferrite 5 increases,
The withstand voltage of the MFS begins to decrease rapidly. Therefore, by utilizing such characteristics, it is possible to open and close the partition walls due to temperature changes caused by the magnetic fluid.

第7図は、第2図例と第5図例のMFSを組合せた構造
((なっている。但し、ポールピース2の間の感温フェ
ライトのキュリ一点はTc、、ポールピース2と永久磁
石1との間の感温フェライトのキュリ一点TC2とし、
しかも’f”c、 (Tc、の関係に設定している。従
って、Tc、以下の温度では感温フェライト51に主に
永久磁石1から発生した磁束が通るので耐圧力は発生し
ない。またTc、近傍の温度から磁性流体3を通過する
磁束の量が増えるので、耐圧が増加していく。TC2近
傍になると感温フェライト52の起磁力損失が大きくな
るので、磁性流体3を通過する磁束量が低下し耐圧が急
激(で落ちる。この関係を線図で表わすと第8図の如く
になる。従って、本例においては、Tc。
Figure 7 shows a structure in which the MFSs of the example in Figure 2 and the example in Figure 5 are combined. Assume one point TC2 of temperature-sensitive ferrite between 1 and 1,
Furthermore, the relationship 'f'c, (Tc) is set. Therefore, at temperatures below Tc, the magnetic flux mainly generated from the permanent magnet 1 passes through the temperature-sensitive ferrite 51, so no withstand pressure is generated. , the amount of magnetic flux passing through the magnetic fluid 3 increases from the nearby temperature, so the withstand voltage increases.As the temperature approaches TC2, the magnetomotive force loss of the temperature-sensitive ferrite 52 increases, so the amount of magnetic flux passing through the magnetic fluid 3 increases. decreases, and the withstand voltage drops rapidly. This relationship can be expressed in a diagram as shown in FIG. 8. Therefore, in this example, Tc.

〜TC2の温度領域でのみ磁性流体((よる流路遮断が
可能となり、所謂バルブ機能を有すること尾なる。
The flow path can be blocked by magnetic fluid only in the temperature range of ~TC2, and it has a so-called valve function.

第9図は基本的には第2図例と第5図例のMl”Sを組
合せた構造になっているが、感温フェライト61.62
のキュリ一点をそれぞれTc、 、 Tc2とすると、
Tc、(、Tc2なる関係になっている。
The structure shown in FIG. 9 is basically a combination of Ml"S in the example in FIG. 2 and the example in FIG.
Let the points of Curie be Tc, , Tc2 respectively,
The relationship is Tc, (, Tc2.

従って、Tc、以下の温度では永久磁石1から発生する
磁束は2つの磁路を形成することになる。
Therefore, at a temperature below Tc, the magnetic flux generated from the permanent magnet 1 will form two magnetic paths.

1つは永久磁石1→ポ一ルピース21→感温フエライト
62→ポールピース22→永久磁石1(以下第1路とい
う)。もう1つは永久磁石1→感温フ工ライト61→ポ
ールピース21→回転軸4→ポールピース22→永久磁
石1(以下第2路という)。この場合は第2路による磁
束で耐圧が発生している。Tc、近傍の温度になると、
第1路にある感温フェライト62の起磁力損失が大きく
なり、第2路を磁束は通過【2な(なり、耐圧が急激に
下がり始める。次く、TC2近傍1(なると、第1路を
磁束が通過できなくなるから、第1路の磁束は永久磁石
1→ポ一ルピース21→回1販軸4→ポールピース22
→永久磁石1という経路をとり耐圧が発生する(第10
図参照)。
One is permanent magnet 1 → pole piece 21 → temperature-sensitive ferrite 62 → pole piece 22 → permanent magnet 1 (hereinafter referred to as the first path). The other path is permanent magnet 1 → temperature-sensitive light 61 → pole piece 21 → rotating shaft 4 → pole piece 22 → permanent magnet 1 (hereinafter referred to as the second path). In this case, the withstand voltage is generated by the magnetic flux caused by the second path. When the temperature approaches Tc,
The magnetomotive force loss of the temperature-sensitive ferrite 62 in the first path increases, and the magnetic flux passes through the second path [2], and the withstand voltage begins to drop rapidly. Since the magnetic flux cannot pass through, the magnetic flux in the first path is permanent magnet 1 → pole piece 21 → rotation 1 sales shaft 4 → pole piece 22
→The path of permanent magnet 1 is taken and withstand voltage is generated (10th
(see figure).

従って、本発明は密封装置の耐圧を温度により自由に変
化することもできるので、流体のA整弁のような装置と
しても多くの応用に適用することかできるう 尚、本発明は回転軸に代えて回転しない軸とすることか
でき、また回転軸の径を無限大にした平板になった場合
でも適用し得る。更に、上述例においては感温磁性体を
付すロする構成であるが、その付加をすることなく環状
ポールピース又は回転軸自体な感温磁性体で構成しても
良いことは勿論である。
Therefore, since the present invention can freely change the pressure resistance of the sealing device depending on the temperature, it can be applied to many applications as a device such as a fluid A control valve. Alternatively, a non-rotating shaft can be used, and it can also be applied to a flat plate with an infinitely large diameter. Further, in the above example, the temperature-sensitive magnetic material is attached, but it goes without saying that the annular pole piece or the rotating shaft itself may be made of the temperature-sensitive magnetic material without the addition of the temperature-sensitive magnetic material.

以上述べた如く本発明によれば、軸、該軸と間隙を有し
て対向しかつ両極間に磁路を形成する磁石装置及び上記
間隙を所定の個所で閉塞する流動性を有する磁性流体で
構成される密封装置において、前記磁路の途中あるいは
その磁路に隣接する個所が感温磁性体で構成したので、
環境温度の変動があっても密封装置内の耐圧を一定又は
増加することができる。従って、環境温度の変動があっ
ても、密封装置内の磁性流体が密封装置外部へ流出せず
、磁性流体を使った高信頼性の密封装置(MFS)を提
供することができる。また、本発明MFSは、耐圧の対
温度特性を自由に変化設定し得るので、エア弁等の開閉
機構として多方面に利用することができる。
As described above, the present invention includes a shaft, a magnet device facing the shaft with a gap therebetween and forming a magnetic path between the two poles, and a magnetic fluid having fluidity that closes the gap at a predetermined location. In the constructed sealing device, since the part in the middle of the magnetic path or the part adjacent to the magnetic path is made of a temperature-sensitive magnetic material,
Even if there are fluctuations in the environmental temperature, the withstand pressure within the sealing device can be kept constant or increased. Therefore, even if the environmental temperature fluctuates, the magnetic fluid inside the sealing device will not flow out of the sealing device, and a highly reliable sealing device (MFS) using magnetic fluid can be provided. Furthermore, since the MFS of the present invention can freely change and set the withstand pressure and temperature characteristics, it can be used in many ways as an opening/closing mechanism for air valves and the like.

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

第1図は磁i11流体シール装置の基本構造断面図、第
2Iン1は木兄・すjの一例を示す断面図、第3図は本
発明の作用効果の説明に供する耐圧一温度特注線図、第
4図は本発明の第2例を示す1新面図、第5図は本発明
の第3例を示す断面図、第6図は第5図例の耐圧一温度
特性、4図、第7図は本発明の第4例を示す断面図、第
8図は第7図例の耐圧一温度特性線図、第9図は本発明
の第5例を示す断面図、第10図は$9図例の耐圧一温
度特性線図である。 1・・・永久磁石、2・・・ポールピース、3・・・磁
性流体、4・・回転軸、5 ・感温磁性材料出願人代理
人 燐埋士 秋 山 高 第3図 第ど図 7cm ′/望度CT) 第7図 第8図 第9図 に2 第10図
Fig. 1 is a cross-sectional view of the basic structure of the magnetic i11 fluid seal device, No. 2 I-1 is a cross-sectional view showing an example of Kinoe Suj, and Fig. 3 is a pressure-resistant-temperature custom-made wire for explaining the effects of the present invention. Figure 4 is a new view showing a second example of the present invention, Figure 5 is a sectional view showing a third example of the present invention, Figure 6 is a breakdown voltage-temperature characteristic of the example in Figure 5, and Figure 4 is a new view showing a second example of the present invention. , FIG. 7 is a sectional view showing a fourth example of the present invention, FIG. 8 is a breakdown voltage-temperature characteristic diagram of the example in FIG. 7, FIG. 9 is a sectional view showing a fifth example of the present invention, and FIG. 10 is a breakdown voltage-temperature characteristic diagram of the $9 example. 1...Permanent magnet, 2...Pole piece, 3...Magnetic fluid, 4...Rotating shaft, 5 - Temperature-sensitive magnetic material applicant's agent Taka Akiyama, Phosphorus Figure 3, Figure 7cm '/Visibility CT) Figure 7 Figure 8 Figure 9 and 2 Figure 10

Claims (1)

【特許請求の範囲】[Claims] 軸、該軸と間隙を有(−て対向しがっ両極間に磁路を形
成する磁石装置及び−1−記間隙を所定の個所で閉塞す
る流動性を有する磁性流体で構成される密封装置におい
て、前記磁路の途中あるいはその磁路に隣接する個所が
感温磁性体で構成したことを特徴とする密封装置。
a shaft, a magnet device that has a gap with the shaft (-) and forms a magnetic path between the opposing poles, and -1- a sealing device that is made of a magnetic fluid with fluidity that closes the gap at a predetermined location. A sealing device characterized in that a portion in the middle of the magnetic path or adjacent to the magnetic path is made of a temperature-sensitive magnetic material.
JP58175040A 1983-09-20 1983-09-20 Sealing device Granted JPS6066362A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58175040A JPS6066362A (en) 1983-09-20 1983-09-20 Sealing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58175040A JPS6066362A (en) 1983-09-20 1983-09-20 Sealing device

Publications (2)

Publication Number Publication Date
JPS6066362A true JPS6066362A (en) 1985-04-16
JPH0363149B2 JPH0363149B2 (en) 1991-09-30

Family

ID=15989160

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58175040A Granted JPS6066362A (en) 1983-09-20 1983-09-20 Sealing device

Country Status (1)

Country Link
JP (1) JPS6066362A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6256797U (en) * 1985-09-28 1987-04-08
JPS6273161U (en) * 1985-10-29 1987-05-11

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6256797U (en) * 1985-09-28 1987-04-08
JPS6273161U (en) * 1985-10-29 1987-05-11

Also Published As

Publication number Publication date
JPH0363149B2 (en) 1991-09-30

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