JPS5911773B2 - Static pressure gas bearing device - Google Patents
Static pressure gas bearing deviceInfo
- Publication number
- JPS5911773B2 JPS5911773B2 JP10977680A JP10977680A JPS5911773B2 JP S5911773 B2 JPS5911773 B2 JP S5911773B2 JP 10977680 A JP10977680 A JP 10977680A JP 10977680 A JP10977680 A JP 10977680A JP S5911773 B2 JPS5911773 B2 JP S5911773B2
- Authority
- JP
- Japan
- Prior art keywords
- bearing
- vacuum chamber
- gas
- nozzle
- bearing surface
- 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
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- Magnetic Bearings And Hydrostatic Bearings (AREA)
Description
【発明の詳細な説明】
本発明は軸受剛性を向上した静圧気体軸受に関5 する
。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a hydrostatic gas bearing with improved bearing rigidity.
従来一般に用いられている静圧気体軸受は、例えばジャ
ーナル軸受に付いていえば、被支持体としての回転する
軸にわずかな間隙をもつて対向した軸受面に圧縮気体を
噴出する軸受ノズルを複数10個設けて構成されている
。A conventionally commonly used hydrostatic gas bearing, for example a journal bearing, has a plurality of ten bearing nozzles that eject compressed gas onto a bearing surface that faces a rotating shaft as a supported body with a small gap. It is composed of individual parts.
そしてこの間隙を流れる気体の圧力分布によつて軸を支
持し、軸受剛性は負荷側の圧力と反負荷側の圧力の差を
軸受と軸との間隙の変動によつて発生させることにより
与えられる。またスラスト軸受の場合を第1図によ15
り説明すると、軸1のスラスト荷重を受ける被支持体2
の平坦な被支持面3に対向してスラスト軸受4の平坦な
軸受面5を設け、この軸受面5に開口した複数個の軸受
ノズル6、6から圧縮気体Tを噴出させて、その間隙I
を気体が流れることに20より軸1を支持している。こ
れも外力によつて、その間隙Iの大きさが変動すると、
気体7の圧力が変化し、この外力に反ばつする力が生じ
剛性が与えられる。上述の剛性につき、スラスト軸受を
例に説明す25ると、被支持体2とスラスト軸受4とが
平衡を保つているときに、被支持体2に△fなる外力が
作用し、被支持体2はΔれ変位する。The shaft is supported by the pressure distribution of the gas flowing through this gap, and bearing rigidity is given by creating a difference between the pressure on the load side and the pressure on the anti-load side by varying the gap between the bearing and the shaft. . In addition, the case of thrust bearings is shown in Figure 1.
To explain, the supported body 2 receives the thrust load of the shaft 1.
A flat bearing surface 5 of the thrust bearing 4 is provided opposite to the flat supported surface 3 of the thrust bearing 4, and compressed gas T is ejected from a plurality of bearing nozzles 6, 6 opened in this bearing surface 5 to fill the gap I.
The shaft 1 is supported by 20 through which the gas flows. Also, if the size of the gap I changes due to external force,
The pressure of the gas 7 changes, creating a force that counteracts this external force and providing rigidity. The above-mentioned rigidity will be explained using a thrust bearing as an example. When the supported body 2 and the thrust bearing 4 are in balance, an external force △f acts on the supported body 2, and the supported body 2 is displaced by Δ.
この変位により間隙9が変化して外力△fとは逆方向の
力Δf、が被支持体2に作用して平衡を保つ。これをプ
ロ30 ツク図で示すと第2図のようになる。ここでF
は△fと△れの関係を示す関数であり、Gは△れと△f
0との関係を示す関数である。従つて剛性は△f1+F
G・・・・・・ (1)
△れF
35となる。Due to this displacement, the gap 9 changes, and a force Δf in the opposite direction to the external force Δf acts on the supported body 2 to maintain balance. If this is shown in a professional diagram, it will look like Figure 2. Here F
is a function that shows the relationship between △f and △re, and G is a function that shows the relationship between △re and △f
This is a function that shows the relationship with 0. Therefore, the stiffness is △f1+F
G... (1) △Less F 35.
気体軸受の剛性は大略式(1)で表かされるが、一般に
高精度で、摩擦が小さいというすぐれた特徴をそなえて
いるが、剛性が小さいという欠点があり、これの向上が
望まれている。The rigidity of gas bearings is roughly expressed by formula (1), and although they generally have excellent characteristics of high precision and low friction, they have the disadvantage of low rigidity, and it is desired to improve this. There is.
本発明は上述の事情にかんがみてなされたもので、静圧
気体軸受の軸受面に軸を支持する軸受ノズルを設けると
ともに、軸に対して互に対称の位置に真空室を設け、こ
れらの吸引力を軸受ノズルからの気体の流出量の変化に
より調節することにより剛性を向上させた静圧気体軸受
である。The present invention has been made in view of the above-mentioned circumstances, and includes a bearing nozzle that supports the shaft on the bearing surface of a hydrostatic gas bearing, vacuum chambers that are located symmetrically with respect to the shaft, and vacuum chambers that support the shaft. This is a hydrostatic gas bearing with improved rigidity by adjusting the force by changing the amount of gas flowing out from the bearing nozzle.
以下本発明の詳細を、第3図ないし第5図に示す一実施
例により説明する〇本実施例はジヤーナル静圧気体軸受
に本発明を適用したものである。The details of the present invention will be explained below with reference to an embodiment shown in FIGS. 3 to 5. In this embodiment, the present invention is applied to a journal static pressure gas bearing.
本体11は角プロツク状部材12に被支持体としての軸
1を挿通する軸受孔13を貫通して設けて構成されてい
る。この軸受孔13の内面は軸受面14を形成している
。この軸受面14には一方の端面16側に軸受ノズル1
8,19,20,21が開口しており、他方の端面23
側に軸受ノズル25,26,27,28が開口している
。軸受ノズル18,19,20,21は、軸1が水平方
向に延在しているので、同一鉛直面内に上下左右に90
度ずつ等配に離間して開口していて、他端は一方の端面
16にそれぞれ開口している。これらの端面16の開口
18a,19a,20a,21aから圧縮気体7が導入
され、軸受ノズル18,19,20,21から噴出して
軸1を支持する。また他方の端面17側の軸受ノズル2
5,26,27,28も同様などで詳細な説明は省略す
るが、他方の端面17の開口25a,26a,27a,
28aから圧縮気体7が導入され軸受ノズル25,26
,27,28から噴出して軸1を支持する。軸1を介し
て対向した一方の側の軸受面31および他方の側の軸受
面32にはそれぞれの面に開口した凹所からなる真空室
34,35が設けられている。これらは本体11に取付
けられた減圧体36,37に連通している。この減圧体
36,37は挟小部38,39をもつた気体流路40,
41、いわゆるラバウル状ノズルに圧縮気体42を流し
て減圧を得るものである。真空室34,35はこれら気
体流路40,41に連通していて、常に軸受間隙におけ
る気体圧力よりはるかに低圧に保たれている。なお真空
室34,35は一般の真空ポンプなどの真空装置に接続
しておいてもよいことはいうまでもないことである。こ
の真空室34と軸受ノズル18,25との間には一方の
側の軸受面31に開口した円弧状の案内溝44,45が
設けられていて、これら案内溝44,45は一方の端が
軸受面31に沿つて延びて、他方側の軸受面32の真空
室35に連通している。そして軸受ノズル18と一端面
16との間および軸受ノズル25と他端面17との間に
は上述の案内溝44,45と同様な円弧状の案内溝46
,47が設けられていて、これらは本体11内において
案内溝44,45にそれぞれ連通している。これらの案
内溝44,45,46,47により軸受ノズル18,2
5から噴出する圧縮気体(空気)7は吸引されて真空室
35に入り、さらに減圧体37を経て大気に放出される
。一方、他方の側の軸受面32にも真空室35と軸受ノ
ズル20,27との間に案内溝50,51が設けられて
おり、さらにまた一端面16と軸受ノズル20との間お
よび他端面17と軸受ノズル27との間にもそれぞれ案
内溝52,53が設けられている。これら案内溝50,
51,52,53は真空室34に連通して、案内溝44
,45,46,47に対応して設けられたもので、同様
な作用をもつているおり、説明は省略する。次に作動に
つき説明する。The main body 11 is constructed by providing a square block-like member 12 with a bearing hole 13 through which a shaft 1 as a supported body is inserted. The inner surface of this bearing hole 13 forms a bearing surface 14 . This bearing surface 14 has a bearing nozzle 1 on one end surface 16 side.
8, 19, 20, 21 are open, and the other end surface 23
Bearing nozzles 25, 26, 27, 28 are open on the sides. Since the shaft 1 extends in the horizontal direction, the bearing nozzles 18, 19, 20, and 21 are arranged at 90° vertically and horizontally within the same vertical plane.
The openings are spaced apart from each other at equal intervals, and the other end is opened at one end surface 16, respectively. Compressed gas 7 is introduced through openings 18a, 19a, 20a, and 21a in these end faces 16, and is ejected from bearing nozzles 18, 19, 20, and 21 to support shaft 1. Also, the bearing nozzle 2 on the other end face 17 side
The openings 25a, 26a, 27a, and
Compressed gas 7 is introduced from 28a to bearing nozzles 25, 26.
, 27, 28 to support the shaft 1. A bearing surface 31 on one side and a bearing surface 32 on the other side facing each other via the shaft 1 are provided with vacuum chambers 34 and 35 each consisting of a recess opened in each surface. These communicate with pressure reducing bodies 36 and 37 attached to the main body 11. The pressure reducing bodies 36 and 37 are connected to a gas flow path 40 having narrow portions 38 and 39,
41, compressed gas 42 is passed through a so-called Rabaul-shaped nozzle to obtain reduced pressure. The vacuum chambers 34, 35 communicate with these gas channels 40, 41 and are always kept at a much lower pressure than the gas pressure in the bearing gap. It goes without saying that the vacuum chambers 34 and 35 may be connected to a vacuum device such as a general vacuum pump. Between the vacuum chamber 34 and the bearing nozzles 18, 25 are provided arcuate guide grooves 44, 45 which are open to the bearing surface 31 on one side, and these guide grooves 44, 45 have one end. It extends along the bearing surface 31 and communicates with the vacuum chamber 35 of the other bearing surface 32 . And between the bearing nozzle 18 and one end surface 16 and between the bearing nozzle 25 and the other end surface 17 are arc-shaped guide grooves 46 similar to the above-mentioned guide grooves 44 and 45.
, 47 are provided, which communicate with the guide grooves 44, 45, respectively, within the main body 11. These guide grooves 44, 45, 46, 47 allow the bearing nozzles 18, 2
Compressed gas (air) 7 ejected from 5 is sucked and enters the vacuum chamber 35, and is further discharged to the atmosphere via a decompression body 37. On the other hand, guide grooves 50 and 51 are provided on the other side of the bearing surface 32 between the vacuum chamber 35 and the bearing nozzles 20 and 27, and also between the one end surface 16 and the bearing nozzle 20 and the other end surface. Guide grooves 52 and 53 are also provided between the bearing nozzle 17 and the bearing nozzle 27, respectively. These guide grooves 50,
51, 52, 53 are in communication with the vacuum chamber 34 and are connected to the guide groove 44.
, 45, 46, and 47, and have similar functions, so the explanation thereof will be omitted. Next, the operation will be explained.
気体(圧縮空気)7を一端面16の開口18a,19a
,20a,21aおよび他端面17の開口25a,26
a,27a,28aから供給して、軸受ノズル18,1
9,20,21および軸受ノズル25,26,27,2
8から噴出させる。そして減圧体36,37の気体流路
40,41に圧縮気体(空気)42を供給すると、これ
らは挟小部38,39で断熱膨脹して圧力が降下するの
で、真空室34,35は真空状態に減圧される。これに
より軸受ノズル18,25から噴出した気体7は、案内
溝46,44および案内溝47,45に吸引され、真空
室35に入り減圧体37を通つて大気に放出される。軸
受ノズル20,27から噴出する圧縮気体(空気)7に
ついても同様に真空室34に入り、減圧体36を経て大
気に放出される。軸受ノズル19,21,26,28か
ら噴出する圧縮気体(空気)7も同様にして適宜真空室
34,35に入り大気に放出される。この状態において
は軸受ノズル18,・・・28からの気体の押圧力、真
空室34,35の吸引力などが軸1に作用し、平衡を保
つて軸受としての機能を発揮する。この状態において、
軸1に上方から下方に向う外力、すなわち矢印55の方
向の外力Δfが作用すると、上方の間隙f!1は大とな
り、下方の間隙G2は小となる。Gas (compressed air) 7 is passed through openings 18a and 19a in one end surface 16.
, 20a, 21a and openings 25a, 26 in the other end surface 17.
a, 27a, 28a, and bearing nozzles 18, 1
9, 20, 21 and bearing nozzles 25, 26, 27, 2
Squirt from 8. When compressed gas (air) 42 is supplied to the gas flow paths 40, 41 of the pressure reducing bodies 36, 37, the compressed gas (air) 42 expands adiabatically in the pinched portions 38, 39 and the pressure drops, so that the vacuum chambers 34, 35 are vacuumed. The state is depressurized. As a result, the gas 7 ejected from the bearing nozzles 18 and 25 is sucked into the guide grooves 46 and 44 and the guide grooves 47 and 45, enters the vacuum chamber 35, passes through the decompression body 37, and is discharged to the atmosphere. The compressed gas (air) 7 ejected from the bearing nozzles 20 and 27 similarly enters the vacuum chamber 34 and is discharged to the atmosphere via the pressure reducing body 36. Similarly, the compressed gas (air) 7 ejected from the bearing nozzles 19, 21, 26, 28 enters the vacuum chambers 34, 35 as appropriate and is discharged to the atmosphere. In this state, the pressing force of gas from the bearing nozzles 18, . In this state,
When an external force Δf in the direction of the arrow 55 acts on the shaft 1 from above to below, the upper gap f! 1 is large, and the lower gap G2 is small.
その結果軸受ノズル18,25からの気体(空気)7の
流量は増加し、このため真空室35に流入する気体(空
気)7は増加し、減圧の程度が低くなり、この部分の吸
引力(矢印55の向き)は減少する。一方下方の軸受ノ
ズル20,27からの気体(空気)7の流量は減少し、
真空室34に流入する気体7の量は減少し、減圧の程度
は高くなり、この部分の吸引力(矢印55と反対の向き
)は増大する。以上の変化をプロツク図で示すと第5図
のようになる。すなわち、上述の外力の変化を△f1こ
れによる間隙9の変化量を△H,△fと△hの関係を表
わす関数をF,△hにより軸受ノズル18,20,25
,27により生じる反発力を△Fl,△hと△F,との
関係を表わす関数をG,Δhにより真空室34に発生す
る吸引力を△F2、同様に真空室35に発生する吸引力
△F3,△hと△F2との関係および△hと△F3との
関係を表わす真空形成の関数をそれぞれVl,,とする
と第5図に示すように、△Fl,△F2,△F3はすべ
て△fとは反対方向に作用しその剛性Δfll+F(j
(1±V1士V2ノは一=
・・・・・・(2)となる。As a result, the flow rate of gas (air) 7 from the bearing nozzles 18, 25 increases, and therefore the amount of gas (air) 7 flowing into the vacuum chamber 35 increases, the degree of pressure reduction decreases, and the suction force ( direction of arrow 55) decreases. On the other hand, the flow rate of gas (air) 7 from the lower bearing nozzles 20, 27 decreases,
The amount of gas 7 flowing into the vacuum chamber 34 decreases, the degree of pressure reduction increases, and the suction force (in the opposite direction to arrow 55) in this area increases. The above changes are shown in a block diagram as shown in FIG. That is, the change in the external force mentioned above is △f1, the amount of change in the gap 9 due to this is △H, the function expressing the relationship between △f and △h is F, and △h is used for the bearing nozzles 18, 20, 25.
, 27 is ΔFl, the function representing the relationship between Δh and ΔF is G, the suction force generated in the vacuum chamber 34 by Δh is ΔF2, and similarly the suction force generated in the vacuum chamber 35 is Δ Assuming that the vacuum formation functions representing the relationship between F3, △h and △F2 and the relationship between △h and △F3 are respectively Vl, , as shown in Figure 5, △Fl, △F2, and △F3 are all It acts in the opposite direction to △f and its stiffness Δfll+F(j
(1±V1 and V2 is one =
...(2).
ΔHFすなわち上述した剛性を表わす(1)式と(2)
式とを比, FG(V1十V2ノ較すれば明らかなよう
に だけ剛F性は大となる。ΔHF, that is, equation (1) representing the above-mentioned stiffness and (2)
If you compare FG (V1 + V2) with the formula, it is clear that the stiffness is greater.
なお軸受内は外力の変化(△f)に対してすきまの変化
(△h)を生じ、外力の変化に相当する内部の圧力変化
を生じて△fに均り合う力を発生する。Note that within the bearing, a change in clearance (△h) occurs in response to a change in external force (△f), and an internal pressure change corresponding to the change in external force is generated to generate a force that is balanced by △f.
これは1種のフイードバツク制御であつて、第2図に示
すような系が成立する。次に本発明について説明する。This is a type of feedback control, and a system as shown in FIG. 2 is established. Next, the present invention will be explained.
第5図において、1,2の系を取ると上記一搬的な軸受
となる。ところで本発明には軸受の上下部に34,35
などの真空室があつて、軸受から流入する流体を排出し
ているが、当然真空室であるので吸引力F2,f3を発
生する。その吸引力は真空度に比例するから、軸受から
流入する流量に反比例する。したがつて、△f→△h→
△f1の一搬軸受作用に加えて″HTZ?7r新たな作
用を生ずる。したがつて、第5図の制御系となる。これ
をまとめると、フとなつて式(2)のようになる。In FIG. 5, if we take the system 1 and 2, we get the above-mentioned uniform bearing. By the way, in the present invention, the upper and lower parts of the bearing have 34 and 35 parts.
There are vacuum chambers such as these to discharge the fluid flowing in from the bearings, and since they are vacuum chambers, they naturally generate suction forces F2 and f3. Since the suction force is proportional to the degree of vacuum, it is inversely proportional to the flow rate flowing from the bearing. Therefore, △f→△h→
In addition to the single-transport bearing action of △f1, a new action of "HTZ?7r" is generated. Therefore, the control system shown in Fig. 5 is obtained.To summarize this, the equation (2) becomes .
以上詳述したように、本発明の静圧気体軸受装置は軸受
ノズルを設けるとともに被支持体を介して一方の側の軸
受面および他方の側の軸受面に真空室を設けて一方の側
の軸受ノズルからの気体を他方の側の真空室で吸引し、
他方の側の軸受ノズルからの気体を一方の側の真空室で
吸引するように構成したので、一方の側の軸受ノズルか
らの気体の流量の増減は他方の側の真空室の吸引力の減
増となるため、従来の剛性にさらにこの真空室により生
じる反発力による剛性が加わり、従来より剛性力が著し
く大となり、外力に対し安定した高精度な軸受が提供で
きる。As described in detail above, the hydrostatic gas bearing device of the present invention is provided with a bearing nozzle, and a vacuum chamber is provided between the bearing surface on one side and the bearing surface on the other side via the supported body. The gas from the bearing nozzle is sucked into the vacuum chamber on the other side,
Since the configuration is such that the gas from the bearing nozzle on the other side is sucked into the vacuum chamber on one side, an increase or decrease in the flow rate of gas from the bearing nozzle on one side will cause a decrease in the suction force in the vacuum chamber on the other side. As a result, the rigidity due to the repulsive force generated by the vacuum chamber is added to the conventional rigidity, and the rigidity is significantly greater than the conventional rigidity, making it possible to provide a high-precision bearing that is stable against external forces.
なお本実施例においてはジヤーナル軸受について記載し
たが、スラスト軸受についても適用されることは云うま
でもない。Although this embodiment has been described with respect to a journal bearing, it goes without saying that the present invention is also applicable to a thrust bearing.
また一般の支持部分についても適用されるものである。It also applies to general support parts.
第1図は従来例の要部を示す一部断面正面図、第2図は
従来例の剛性を説明するプロツク図、第3図は本発明の
一実施例の断面正面図、第4図は第3図のIV−1V断
面を矢視方向に見た断面図、第5図は本発明の一実施例
の剛性を説明するプロツク図である。
1,2:被支持体、7:気体、14:軸受面、16:ー
方の端面、17:他方の端面、18,19,20,21
,25,26,27,28:軸受ノズル、31:ー方の
側の軸受面、32:他方の側の軸受面、34:ー方の真
空室、35:他方の真空室、44,45,46,47:
ー方の案内溝、50,51,52,53:他方の案内溝
。FIG. 1 is a partially sectional front view showing the main parts of the conventional example, FIG. 2 is a block diagram explaining the rigidity of the conventional example, FIG. 3 is a sectional front view of an embodiment of the present invention, and FIG. FIG. 3 is a sectional view taken along the line IV-1V in the direction of the arrow, and FIG. 5 is a block diagram for explaining the rigidity of an embodiment of the present invention. 1, 2: Supported body, 7: Gas, 14: Bearing surface, 16: - side end face, 17: Other end face, 18, 19, 20, 21
, 25, 26, 27, 28: Bearing nozzle, 31: Bearing surface on the - side, 32: Bearing surface on the other side, 34: Vacuum chamber on the - side, 35: Vacuum chamber on the other side, 44, 45, 46, 47:
- guide grooves, 50, 51, 52, 53: guide grooves on the other side.
Claims (1)
する複数個の軸受ノズルと、上記被支持体を介して対向
した一方の側の上記軸受面に開口し真空源に連通した一
方の真空室と、上記軸を介して対向した他方の側の上記
軸受面に開口し真空源に連通した他方の真空室と、上記
一方の側の軸受面に設けられかつ上記他方の真空室に連
通し上記一方の側の軸受面の軸受ノズルから噴出する上
記気体を上記他方の真空室に導く一方の案内溝と、上記
他方の側の軸受面に設けられかつ上記一方の真空室に連
通し上記他方の側の軸受面の軸受ノズルから噴出する上
記気体を上記一方の真空室に導く他方の案内溝とを具備
したことを特徴とする静圧気体軸受装置。 2 一方の案内溝は一方の側の軸受面に設けられた最外
側の軸受ノズルと端面との間および最内側の軸受ノズル
と一方の真空室との間に設けられており、他方の案内溝
は他方の側の軸受面に設けられた最外側の軸受ノズルと
端面との間および最内側の軸受ノズルと他方の真空室と
の間に設けられていることを特徴とする特許請求の範囲
第1項記載の静圧気体軸受装置。[Scope of Claims] 1. A plurality of bearing nozzles that are provided on a bearing surface and eject gas to support a supported object, and a plurality of bearing nozzles that are opened in the bearing surface on one side facing each other with the supported object in between, and a vacuum one vacuum chamber that communicates with the vacuum source, the other vacuum chamber that opens in the bearing surface on the other side facing through the shaft and communicates with the vacuum source, and the vacuum chamber that is provided in the bearing surface of the one side and that one guide groove that communicates with the other vacuum chamber and guides the gas ejected from the bearing nozzle on the one bearing surface to the other vacuum chamber; A static pressure gas bearing device comprising: a second guide groove that communicates with a vacuum chamber and guides the gas ejected from a bearing nozzle on the other bearing surface to the one vacuum chamber. 2 One guide groove is provided between the outermost bearing nozzle provided on the bearing surface on one side and the end face, and between the innermost bearing nozzle and one vacuum chamber, and the guide groove on the other side is provided between the outermost bearing nozzle and the end face. is provided between the outermost bearing nozzle provided on the other side bearing surface and the end face, and between the innermost bearing nozzle and the other vacuum chamber. The static pressure gas bearing device according to item 1.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10977680A JPS5911773B2 (en) | 1980-08-12 | 1980-08-12 | Static pressure gas bearing device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10977680A JPS5911773B2 (en) | 1980-08-12 | 1980-08-12 | Static pressure gas bearing device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5737118A JPS5737118A (en) | 1982-03-01 |
| JPS5911773B2 true JPS5911773B2 (en) | 1984-03-17 |
Family
ID=14518931
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10977680A Expired JPS5911773B2 (en) | 1980-08-12 | 1980-08-12 | Static pressure gas bearing device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5911773B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP3949910B2 (en) * | 2001-07-05 | 2007-07-25 | 株式会社ミツトヨ | Drive device using air bearing |
-
1980
- 1980-08-12 JP JP10977680A patent/JPS5911773B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5737118A (en) | 1982-03-01 |
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