JPH0733848B2 - Porous static pressure gas bearing - Google Patents
Porous static pressure gas bearingInfo
- Publication number
- JPH0733848B2 JPH0733848B2 JP3085835A JP8583591A JPH0733848B2 JP H0733848 B2 JPH0733848 B2 JP H0733848B2 JP 3085835 A JP3085835 A JP 3085835A JP 8583591 A JP8583591 A JP 8583591A JP H0733848 B2 JPH0733848 B2 JP H0733848B2
- Authority
- JP
- Japan
- Prior art keywords
- porous
- bearing
- flow rate
- static pressure
- gas bearing
- 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
Links
Description
【0001】[0001]
【産業上の利用分野】本発明は多孔質セラミックスを使
用した静圧気体軸受けに関し、特に安定かつ高剛性な多
孔質気体軸受に関するものである。スライシングマシン
は、セラミックスの切断や溝入れ等に用いられる工作機
械であって、その砥石を回転させるスピンドルは加工物
に合った回転数で高速回転しかつ高剛性を得るため、工
場で容易に得られる最大給気圧力で運転される。本発明
の軸受けは、このような安定した高速回転かつ高剛性が
必要なところの軸受けとして利用できる。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a static pressure gas bearing using porous ceramics, and more particularly to a stable and highly rigid porous gas bearing. The slicing machine is a machine tool used for cutting and grooving ceramics, and the spindle that rotates the grindstone rotates at a high speed at a speed suitable for the workpiece and has high rigidity, so it can be easily obtained at the factory. Operates at maximum supply pressure The bearing of the present invention can be used as a bearing where such stable high speed rotation and high rigidity are required.
【0002】[0002]
【従来の技術】従来、軸受け面に多孔質体を配してこの
多孔質体を通して軸受け面の間隙に加圧気体を供給し
て、軸受け面の空気層により軸構造体を保持する多孔質
静圧気体軸受けが知られている。2. Description of the Related Art Conventionally, a porous body is disposed on a bearing surface, pressurized gas is supplied to the gap between the bearing surfaces through the porous body, and an air layer on the bearing surface holds the shaft structure. Pressure gas bearings are known.
【0003】この多孔質体の材料として、従来から多孔
質である焼結金属、カーボンやセラミックスが使用され
ている。このうち、多孔質の焼結金属または多孔質のカ
ーボンを使用した場合は、軸受け面の加工により軸受け
面に目つぶれが生じるため、膨大な工数のかかる再加工
をしなければ、安定で高剛性な静圧気体軸受けを得るこ
とができない問題があった。Porous sintered metal, carbon and ceramics have been conventionally used as the material for the porous body. Of these, if porous sintered metal or porous carbon is used, the bearing surface will be crushed and the bearing surface will be crushed. There was a problem that it was not possible to obtain a proper static pressure gas bearing.
【0004】[0004]
【発明が解決しようとする課題】その点、多孔質セラミ
ックスを使用した場合は上述した目つぶれの問題は発生
しない。しかしながら、例えば、日本機械学会論文集C
編55巻511 号「多孔質セラミックス静圧空気軸受の負荷
特性」に開示されているように、多孔質セラミックスを
使用した静圧気体軸受けでは、自励振動(ニューマチッ
クハンマ)発生による不安定性を有しており、極めて限
定された条件下でしか安定せず、実際に高剛性で安定な
静圧気体軸受けを量産することができない問題があっ
た。On the other hand, when the porous ceramics are used, the above-mentioned problem of the blinding does not occur. However, for example, the Japan Society of Mechanical Engineers, Proceedings C
As disclosed in Vol. 55, No. 511, "Load Characteristics of Porous Ceramics Static Pressure Air Bearings", static pressure gas bearings using porous ceramics are subject to instability caused by self-excited vibration (pneumatic hammer). However, it has a problem that it is stable only under extremely limited conditions, and that it is impossible to mass-produce a highly rigid and stable static pressure gas bearing.
【0005】本発明の目的は上述した課題を解消して、
安定で高剛性な静圧気体軸受けを量産可能な構造を有す
る多孔質静圧気体軸受を提供しようとするものである。The object of the present invention is to solve the above problems,
An object of the present invention is to provide a porous static pressure gas bearing having a structure capable of mass-producing stable and highly rigid static pressure gas bearings.
【0006】[0006]
【課題を解決するための手段】本発明の多孔質静圧軸受
は、軸受け面に、単位面積当りの流量Q[s1/(min ・cm
2 ) ]が、 10-3(0.01P2 +0.02P −0.03) ≦Q≦0.01P2+0.02P −0.03 ----(1) 但し、P:給気圧[kgf/cm2 ・G]である多孔質セラミ
ックスを用いたことを特徴とするものである。In the porous hydrostatic bearing of the present invention, the flow rate per unit area Q [s1 / (min.cm
2 )] is 10 -3 (0.01P 2 + 0.02P -0.03) ≤Q ≤0.01P 2 + 0.02P -0.03 ---- (1) where P: Supply pressure [kgf / cm 2 · G] It is characterized by using the porous ceramics.
【0007】[0007]
【作用】上述した構成において、軸受け面の多孔質セラ
ミックスの単位面積当りに流れる流量を所定の値以下に
すれば、後述する実施例から明らかなように、多孔質セ
ラミックスの他の特性がどうであっても通常の使用にお
いて自励振動が発生せず、安定で高剛性な多孔質静圧気
体軸受を得ることができることを見いだしたことによ
る。In the above-mentioned structure, if the flow rate per unit area of the porous ceramics on the bearing surface is set to a predetermined value or less, as will be apparent from the examples described later, the other characteristics of the porous ceramics may not be affected. This is because it was found that self-excited vibration does not occur in normal use, and a stable and highly rigid porous hydrostatic gas bearing can be obtained.
【0008】なお、下限については特に規定するもので
はないが、Q=10-3(0.01P2 +0.02P −0.03)未満で
は、剛性が小さく軸受として使用できなくなることが多
いので、下限はQ=10-3(0.01P2 +0.02P −0.03)まで
であると好ましい。The lower limit is not specified, but if Q is less than 10 -3 (0.01P 2 + 0.02P -0.03), the rigidity is low and the bearing cannot be used in many cases, so the lower limit is Q. = Up to 10 -3 (0.01P 2 + 0.02P -0.03) is preferable.
【0009】また、所定の通気率を有する多孔質セラミ
ックスを得るためには、粉末を調製し、成形、焼成して
焼結体を得る通常の製造法において、成形時の成形圧を
変化させるか、あるいは焼成時の焼成温度を変化させる
と、簡単に再現性良く所望の通気率を得ることができる
ことを見いだした。Further, in order to obtain a porous ceramics having a predetermined air permeability, it is necessary to change the molding pressure at the time of molding in the usual manufacturing method of preparing powder, molding and firing to obtain a sintered body. It was found that the desired air permeability can be easily obtained with good reproducibility by changing the firing temperature during firing.
【0010】なお、本発明においては多孔質セラミック
スの単位面積当りに流れる流量が上記(1)式を満たす
ものであれば他の特性はどの様なものでも可能だが、こ
の流量を達成するためには、多孔質セラミックスの特性
は通常以下の範囲にある。すなわち、平均細孔径:0.5
〜10μm 、開気孔率:10〜30% 、細孔容積:0.02〜0.08
cc/g、吸水率:2 〜8%、成形密度:2〜5g/cc の範囲に
ある。In the present invention, any other characteristics are possible as long as the flow rate per unit area of the porous ceramics satisfies the above equation (1), but in order to achieve this flow rate, The characteristics of porous ceramics are usually in the following ranges. That is, the average pore diameter: 0.5
~ 10 μm, open porosity: 10-30%, pore volume: 0.02-0.08
cc / g, water absorption: 2-8%, molding density: 2-5 g / cc.
【0011】[0011]
【実施例】図1は本発明の多孔質静圧気体軸受の一例の
構成を示す断面図である。図1において、1は所定の流
量を有する多孔質セラミックス層、2は多孔質セラミッ
クス層1を介して空気等の気体を供給する気体供給部、
3は支持すべき軸構造体である。一般のスライシングマ
シンの砥石スピンドルの軸受寸法は、d=25〜60mm、D
=30〜80mm、1=25〜60mmである。上述した構造の多孔
質静圧気体軸受による軸構造体3の支持は、まず多孔質
セラミックス層1の円筒形状の軸受け面に5〜20μmの
隙間を設けて軸構造体3を装着した後、所定の圧力の気
体を気体供給部2に供給した状態で軸構造体3を回転す
ることにより達成することができる。1 is a sectional view showing the structure of an example of a porous static pressure gas bearing according to the present invention. In FIG. 1, 1 is a porous ceramics layer having a predetermined flow rate, 2 is a gas supply unit for supplying gas such as air through the porous ceramics layer 1,
3 is a shaft structure to be supported. The bearing size of the grindstone spindle of a general slicing machine is d = 25-60mm, D
= 30-80 mm, 1 = 25-60 mm. In order to support the shaft structure 3 by the porous static pressure gas bearing having the above-described structure, first, after mounting the shaft structure 3 with a clearance of 5 to 20 μm provided on the cylindrical bearing surface of the porous ceramic layer 1, a predetermined period is set. This can be achieved by rotating the shaft structure 3 while the gas having the pressure of 1 is supplied to the gas supply unit 2.
【0012】多孔質セラミックス層1は通常のセラミッ
クスの焼成方法、すなわち所定組成の粉末を調製し、調
製した粉末を成形し、成形後の成形体を焼成して得るこ
とができる。その際、後述するように成形時の成形圧を
変化させるか焼成時の焼成温度を変化させることによ
り、所定の流量を有する多孔質セラミックス層1を得る
ことができる。なお、多孔質セラミックス層1は均一な
気孔分布を有し加工しても目づまりしない材料から構成
されると好ましく、多孔質ジルコニア、多孔質アルミ
ナ、多孔質窒化アルミニウム、多孔質炭化ケイ素、多孔
質窒化ケイ素を使用すると好ましい。The porous ceramics layer 1 can be obtained by an ordinary ceramics firing method, that is, by preparing a powder having a predetermined composition, molding the prepared powder, and firing the molded body after molding. At that time, the porous ceramics layer 1 having a predetermined flow rate can be obtained by changing the molding pressure during molding or by changing the baking temperature during baking as described later. The porous ceramics layer 1 is preferably made of a material having a uniform pore distribution and not clogged even when processed, and porous zirconia, porous alumina, porous aluminum nitride, porous silicon carbide, porous Preference is given to using silicon nitride.
【0013】図2は実際の多孔質静圧気体軸受により軸
構造体を受け、自励振動が発生する限界を求めるのに使
用した装置を示す図である。各軸受部の寸法は、d=50
〜60mm、D=55〜75mm、1=50〜60mmの範囲にある。図
2に示す装置では、図1と同様の構造の多孔質静圧気体
軸受に、距離測定センサと加速度ピックアップ4及びFF
Tアナライザー5を設け、各回転数で回転させた時の振
動を計測し、回転数と同期しない周波数成分が発生した
ときに自励振動が発生したものとみなしている。なお、
図1の気体供給部から供給する圧力は7kgf /cm2 Gと
した。これは、給気圧が高い方が軸受剛性が高くなるこ
とと、工場内で容易に供給できる最高圧力であるためで
ある。FIG. 2 is a diagram showing an apparatus used to determine the limit at which self-excited vibration is generated by receiving a shaft structure by an actual porous hydrostatic gas bearing. The size of each bearing is d = 50
-60 mm, D = 55-75 mm, 1 = 50-60 mm. In the device shown in FIG. 2, a distance measuring sensor, an acceleration pickup 4 and an FF are provided in a porous static pressure gas bearing having the same structure as in FIG.
The T-analyzer 5 is provided, the vibration when rotating at each rotation speed is measured, and it is considered that the self-excited vibration is generated when the frequency component that is not synchronized with the rotation speed is generated. In addition,
The pressure supplied from the gas supply unit in FIG. 1 was 7 kgf / cm 2 G. This is because the higher the supply pressure, the higher the bearing rigidity and the maximum pressure that can be easily supplied in the factory.
【0014】実際に図2に示す装置により、多孔質セラ
ミックス層1の単位面積当りに流れる流量を変えてその
際の自励振動の発生する回転数を求めたところ、図3に
示す結果を得た。図3において、数字は試験No. を示す
とともに、数字の枠の意味は、□:2000rpm 以下で、回
転数に同期しない振動成分が発生した軸受の流量曲線
を、Δ:2000rpm 以上30000rpm以下で、回転数に同期し
ない振動成分が発生した軸受の流量曲線を、○:30000r
pmまで、回転数に同期しない振動成分が発生しなかった
軸受の流量曲線を意味し、さらに二重の枠は境界条件と
なる流量曲線を示している。図3から明らかなように、
単位面積当りに流れる流量QをQ=0.01P2+ 0.02P−0.
03以下にしさえすれば、自励振動のない安定した多孔質
静圧気体軸受が得られることがわかる。また、単位面積
当りの流量QがQ=1.2 ×10-3P2+0.01P −7.8 ×10-3
以下であれば、実験で確認できた装置の最高回転数であ
る3万回転まで安定なため、より一層安定な多孔質静圧
気体軸受が得られることがわかる。一方、剛性は、(1)
式を満たすすべての条件で15kgf/μm 以上であることが
実測された。The flow rate per unit area of the porous ceramics layer 1 was actually changed by the apparatus shown in FIG. 2 to find the number of revolutions at which self-excited vibration occurred, and the result shown in FIG. 3 was obtained. It was In Fig. 3, the numbers indicate the test No., the meaning of the frame of the numbers is □: 2000 rpm or less, and the flow rate curve of the bearing in which the vibration component which is not synchronized with the rotation speed occurs is Δ: 2000 rpm or more and 30000 rpm or less, The flow rate curve of the bearing where the vibration component not synchronized with the rotation speed is
Up to pm, it means the flow rate curve of the bearing in which the vibration component not synchronized with the rotation speed did not occur, and the double frame shows the flow rate curve which is the boundary condition. As is clear from FIG.
The flow rate Q flowing per unit area is Q = 0.01P 2 + 0.02P-0.
It can be seen that a stable porous hydrostatic gas bearing without self-excited vibration can be obtained if the amount is 03 or less. In addition, the flow rate Q per unit area is Q = 1.2 × 10 -3 P 2 + 0.01P -7.8 × 10 -3
In the following cases, it can be seen that a more stable porous hydrostatic gas bearing can be obtained because it is stable up to 30,000 rotations, which is the maximum rotation speed of the device confirmed by the experiment. On the other hand, the rigidity is (1)
It was measured to be 15 kgf / μm or more under all conditions that satisfy the formula.
【0015】また、多孔質セラミックス層1の製造時の
成形圧力及び焼成温度の影響を調べるため、同一組成の
セラミックスに対して成形時の成形圧力及び焼成温度を
変化させ、他の条件は同一として多孔質セラミックスを
製造し、その流量を調べたところ、成形圧力及び焼成温
度を変化させることにより、流量を制御することがで
き、この方法が本発明の所定の流量を有する多孔質セラ
ミックスを得るために最適であることがわかったが、成
形圧力と焼成温度は密接な関係にあるため、実際の通気
率の制御にあたっては、これらの間の関係をも考慮する
必要がある。Further, in order to investigate the influence of the molding pressure and the firing temperature at the time of manufacturing the porous ceramics layer 1, the molding pressure and the firing temperature at the time of molding are changed for ceramics of the same composition, and the other conditions are the same. When porous ceramics were manufactured and the flow rate thereof was investigated, the flow rate can be controlled by changing the molding pressure and the firing temperature, and this method is for obtaining the porous ceramics having the predetermined flow rate of the present invention. However, since the molding pressure and the firing temperature are closely related to each other, it is necessary to consider the relationship between them when controlling the actual air permeability.
【0016】[0016]
【発明の効果】以上詳細に説明したところから明らかな
ように、本発明によれば、多孔質静圧気体軸受の多孔質
セラミックス層の単位面積当りに流れる流量さえ上記
(1) 式を満たすように制御すれば、セラミックスを使用
した靜圧気体軸受においても自励振動のない安定かつ高
剛性な軸受を得ることができる。また、上述したセラミ
ックス層の流量の制御には、成形圧力を変化させるか焼
成温度を変化させることにより、簡単に所定の通気率を
有する多孔質セラミックス層を得ることができる。As is apparent from the above detailed description, according to the present invention, even the flow rate per unit area of the porous ceramics layer of the porous static pressure gas bearing is as described above.
By controlling so as to satisfy the formula (1), it is possible to obtain a stable and highly rigid bearing free from self-excited vibration even in a pressurized gas bearing using ceramics. Further, in controlling the flow rate of the ceramic layer described above, the porous ceramic layer having a predetermined air permeability can be easily obtained by changing the molding pressure or the firing temperature.
【図1】本発明の多孔質靜圧気体軸受の一例の構成を示
す断面図である。FIG. 1 is a cross-sectional view showing the configuration of an example of a porous pressurized gas bearing of the present invention.
【図2】本発明において自励振動の発生を調べる状態を
示す図である。FIG. 2 is a diagram showing a state of checking occurrence of self-excited vibration in the present invention.
【図3】本発明における、多孔質層を流れる単位面積当
りの流量が最高回転数に及ぼす影響を示すグラフであ
る。FIG. 3 is a graph showing the influence of the flow rate per unit area flowing through the porous layer on the maximum rotation speed in the present invention.
1 多孔質セラミックス層 2 気体供給部 3 軸構造体 4 距離測定センサ及び加速度ピックアップ 5 FFT アナライザー 1 Porous Ceramics Layer 2 Gas Supply Section 3 Axis Structure 4 Distance Measuring Sensor and Accelerometer 5 FFT Analyzer
Claims (1)
/(min ・cm2 )]が、10-3(0.01P2 +0.02P −0.03) ≦
Q≦0.01P2+0.02P −0.03(但し、P:給気圧[kgf/cm
2 ・G])である多孔質セラミックスを用いたことを特
徴とする多孔質静圧気体軸受。1. A flow rate per unit area Q [s1 on the bearing surface
/ (min ・ cm 2 )] is 10 -3 (0.01P 2 + 0.02P -0.03) ≤
Q ≦ 0.01P 2 + 0.02P −0.03 (However, P: Supply pressure [kgf / cm
Porous hydrostatic gas bearing, characterized in that using a porous ceramic is 2 · G]).
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3085835A JPH0733848B2 (en) | 1991-03-27 | 1991-03-27 | Porous static pressure gas bearing |
EP91310992A EP0488715B1 (en) | 1990-11-29 | 1991-11-28 | A porous hydrostatic gas-bearing |
DE69124730T DE69124730T2 (en) | 1990-11-29 | 1991-11-28 | Porous, gas-static bearing |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3085835A JPH0733848B2 (en) | 1991-03-27 | 1991-03-27 | Porous static pressure gas bearing |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH04300420A JPH04300420A (en) | 1992-10-23 |
JPH0733848B2 true JPH0733848B2 (en) | 1995-04-12 |
Family
ID=13869918
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3085835A Expired - Lifetime JPH0733848B2 (en) | 1990-11-29 | 1991-03-27 | Porous static pressure gas bearing |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0733848B2 (en) |
Family Cites Families (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2566789B2 (en) * | 1986-09-30 | 1996-12-25 | キヤノン株式会社 | Manufacturing method of porous hydrostatic gas bearing |
JPH0289811A (en) * | 1988-09-26 | 1990-03-29 | Ibiden Co Ltd | Static pressure gas bearing |
JPH0281925U (en) * | 1988-12-13 | 1990-06-25 |
-
1991
- 1991-03-27 JP JP3085835A patent/JPH0733848B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPH04300420A (en) | 1992-10-23 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
EP0633406B1 (en) | Combination bearing construction | |
JP3086764B2 (en) | Hydrostatic bearing device | |
EA003437B1 (en) | Method of manufacturing a diamond-silicon carbide-silicon composite and composite produced by this method | |
JP3860253B2 (en) | Static pressure gas bearing | |
JPH05296248A (en) | Slider member | |
US5944427A (en) | Dynamic pressure gas bearing structure and method of manufacturing the same as well as method of using the same | |
JPH0733848B2 (en) | Porous static pressure gas bearing | |
EP0488715A2 (en) | A porous hydrostatic gas-bearing | |
JP3542502B2 (en) | Manufacturing method of hydrostatic porous bearing | |
JP2726776B2 (en) | Grinding method | |
JPH04219519A (en) | Porous static pressure pneumatic bearing | |
JPH04300421A (en) | Porous static pressure gas bearing | |
JP4913468B2 (en) | Silicon carbide polishing plate and method for polishing semiconductor wafer | |
JPH02256915A (en) | Porous static pressure bearing and manufacture thereof | |
JPS6228519A (en) | Ceramic bearing device | |
JP2566789B2 (en) | Manufacturing method of porous hydrostatic gas bearing | |
JPH10103354A (en) | Hydrostatic gas bearing | |
KR100502815B1 (en) | Porous Ceramic Material with Double Pore Structures and Manufacturing Process therefor | |
JP2820400B2 (en) | Drilling method for silicon single crystal | |
JPH0289812A (en) | Static pressure gas bearing | |
JP2892364B2 (en) | Control method of spindle using hydrostatic gas bearing | |
JP2001027240A (en) | Static pressure porous bearing and manufacture thereof | |
JP2000291656A (en) | Manufacture of porous gas hydrostatic bearing | |
JP2000027865A (en) | Static pressure porous bearing | |
JPH1162966A (en) | Hydrostatic bearing and manufacture thereof |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
A02 | Decision of refusal |
Free format text: JAPANESE INTERMEDIATE CODE: A02 Effective date: 19980324 |