[go: up one dir, main page]

CN103352917B - Integrated type air-float guide rail under unbalance loading etc. gap design method - Google Patents

Integrated type air-float guide rail under unbalance loading etc. gap design method Download PDF

Info

Publication number
CN103352917B
CN103352917B CN201310297492.0A CN201310297492A CN103352917B CN 103352917 B CN103352917 B CN 103352917B CN 201310297492 A CN201310297492 A CN 201310297492A CN 103352917 B CN103352917 B CN 103352917B
Authority
CN
China
Prior art keywords
orifice
outlet pressure
guide rail
equal
convergence
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 - Fee Related
Application number
CN201310297492.0A
Other languages
Chinese (zh)
Other versions
CN103352917A (en
Inventor
张君安
宋伟
刘波
杨立芝
方舟
马晨
王娟
赫东锋
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.)
Xian Technological University
Original Assignee
Xian Technological University
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 Xian Technological University filed Critical Xian Technological University
Priority to CN201310297492.0A priority Critical patent/CN103352917B/en
Publication of CN103352917A publication Critical patent/CN103352917A/en
Application granted granted Critical
Publication of CN103352917B publication Critical patent/CN103352917B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Magnetic Bearings And Hydrostatic Bearings (AREA)

Abstract

本发明涉及气浮导轨技术领域,具体涉及一种整体式气浮导轨在偏载下的等间隙设计方法。本发明要克服现有技术存在的导轨在偏载下导向精度低和稳定性差的问题。为克服现有技术存在的问题,本发明所提供的技术方案是:一种整体式气浮导轨在偏载下的等间隙设计方法,其特征在于:改变各节流孔内径大小来实现对导轨由于偏载带来的偏角进行调平。与现有技术相比,利用本发明方法所带来的优点是:与导轨导向垂直方向上由于偏载产生的运动误差在设计理论上被消除了,即仅存在制造误差,相对于现有技术而言,本发明运行精度高,稳定性好。

The invention relates to the technical field of air-floating guide rails, in particular to an equal clearance design method for integral air-floating guide rails under eccentric loads. The invention aims to overcome the problems of low guiding precision and poor stability of the guide rail under partial load in the prior art. In order to overcome the problems existing in the prior art, the technical solution provided by the present invention is: a design method for equal clearance of the integral air-floating guide rail under partial load, which is characterized in that: changing the inner diameter of each orifice to realize the alignment of the guide rail Leveling due to deflection angle caused by eccentric load. Compared with the prior art, the advantage brought by the method of the present invention is that the motion error caused by the eccentric load with the guide rail in the vertical direction is eliminated in design theory, that is, there is only manufacturing error, compared with the prior art In terms of performance, the present invention has high operating precision and good stability.

Description

整体式气浮导轨在偏载下的等间隙设计方法Equal clearance design method of integral air bearing guide rail under eccentric load

技术领域 technical field

本发明涉及气浮导轨技术领域,具体涉及一种整体式气浮导轨在偏载下的等间隙设计方法。 The invention relates to the technical field of air-floating guide rails, in particular to an equal clearance design method for integral air-floating guide rails under eccentric loads.

背景技术 Background technique

用多个气浮垫装配动导轨时,气浮垫用球铰支撑,这样可以自找准平衡位置,保持气膜间隙相等,不过需用到滑架,这时动导轨的体积大承载能力小。而用整体式导轨装配动导轨时,动导轨的体积小承载能力大,而且整体式气浮导轨工作间隙越趋于平行,运行精度越高。但在实际工作过程中发现,现有的整体式气浮导轨还存在着下述的问题:由于载荷或惯性力的作用,整体式气浮导轨在使用过程中必然会产生偏载,若原有导轨间隙为等间隙,则由于偏载必然导致导轨间隙不相等,进而影响运行精度。并且由于气膜厚度很小,很小的偏角就有可能引起刮蹭,影响轴承稳定性,减少轴承的使用寿命。以往针对整体式气浮导轨的设计方法都是以等内径节流孔给气膜供气,这样的设计方法必然使导轨在运行过程中产生偏角问题,降低导轨运行精度和稳定性。 When assembling moving guide rails with multiple air bearing pads, the air bearing pads are supported by ball joints, so that the balance position can be self-aligned and the air film gaps are kept equal. However, a carriage is required, and the moving guide rails are large in size and have a small carrying capacity. . When the integral guide rail is used to assemble the moving guide rail, the moving guide rail has a small volume and a large carrying capacity, and the more parallel the working gap of the integral air bearing guide rail is, the higher the running accuracy is. However, in the actual work process, it is found that the existing integral air-floating guide rails still have the following problems: due to the effect of load or inertial force, the integral air-floating guide rails will inevitably produce unbalanced loads during use. If the gap is equal, the eccentric load will inevitably lead to unequal gaps in the guide rails, which will affect the running accuracy. And because the thickness of the air film is very small, a small deflection angle may cause scratches, affect the stability of the bearing, and reduce the service life of the bearing. In the past, the design method for the integral air bearing guideway was to supply the air film with equal inner diameter orifices. Such a design method would inevitably cause deflection problems during the operation of the guideway, reducing the running accuracy and stability of the guideway.

发明内容 Contents of the invention

本发明要提供一种整体式气浮导轨在偏载下的等间隙设计方法,以克服现有技术存在的导轨运行精度低和稳定性差的问题。 The present invention provides an equal clearance design method for an integral air-floating guide rail under eccentric loads, so as to overcome the problems of low running precision and poor stability of the guide rail in the prior art.

为克服现有技术存在的问题,本发明所提供的技术方案是:一种整体式气浮导轨在偏载下的等间隙设计方法,其特征在于改变各节流孔内径大小来实现对导轨由于偏载带来的偏角进行调平。  In order to overcome the problems existing in the prior art, the technical solution provided by the present invention is: an equal clearance design method of an integral air-floating guide rail under partial load, which is characterized in that the inner diameter of each orifice is changed to realize the adjustment of the guide rail due to The deflection angle brought by the eccentric load is leveled. the

上述整体式气浮导轨在偏载下的等间隙设计方法,包括以下步骤: The equal-gap design method of the above integral air-floating guide rail under partial load includes the following steps:

    一、以长导轨平面为XY坐标平面计算气浮导轨偏载状态下的各个节流孔出口压力,气膜承载力,以及气膜气体压力对X轴与对Y轴的力矩大小; 1. Taking the plane of the long guide rail as the XY coordinate plane to calculate the outlet pressure of each orifice of the air-floating guide rail under the eccentric load state, the bearing capacity of the gas film, and the moment of the gas pressure of the gas film to the X-axis and to the Y-axis;

二、利用雷诺方程以及重积分,计算等间隙状态下气膜承载力和气体对X轴与对Y轴的力矩大小; 2. Using the Reynolds equation and heavy integrals, calculate the gas film bearing capacity and the moment of gas on the X-axis and Y-axis under the equal gap state;

三、以等间隙状态下气膜承载力和偏载力矩与非等间隙状态下都相等为收敛条件,调整节流孔出口压力,得到满足收敛条件的一组节流孔出口压力值; 3. Taking the gas film bearing capacity and eccentric load moment in the equal clearance state as the convergence condition as the non-equal clearance state, adjust the orifice outlet pressure to obtain a set of orifice outlet pressure values that meet the convergence conditions;

四、选取原节流孔内径值为调平后节流孔内径初始值,将XY平面按节流孔个数分为多个区域,分别利用气体流量守恒方程进行嵌套耦合,即以满足各区域进出气体流量相等同时满足整个气膜总进出气体流量相等为收敛条件,若计算过程中某个区域进出气体流量不守恒,则以小步长调节节流孔内径值,直到满足收敛条件。 4. Select the inner diameter of the original orifice as the initial value of the inner diameter of the orifice after leveling, divide the XY plane into multiple areas according to the number of orifices, and use the gas flow conservation equation to perform nested coupling respectively, that is, to satisfy each The convergence condition is that the gas flow in and out of the area is equal and the total gas flow in and out of the entire gas film is equal. If the gas flow in and out of a certain area is not conserved during the calculation process, the inner diameter of the orifice is adjusted in small steps until the convergence condition is met.

上述步骤二中,要求导轨调至等间隙后气膜厚度为调整前受力斜面中心点厚度时,在所述步骤三中,对节流孔出口压力初始值进行调节时,同时增大相应位置气膜厚度变高的节流孔出口压力和减小对应位置气膜厚度变低的节流孔出口压力值,以得到满足力矩收敛条件同时满足厚度要求的一组节流孔出口压力值。 In the above step 2, when the thickness of the air film after the guide rail is adjusted to equal clearance is required to be the thickness of the center point of the stress slope before adjustment, in the above step 3, when adjusting the initial value of the orifice outlet pressure, increase the corresponding position at the same time The orifice outlet pressure at which the gas film thickness becomes higher and the orifice outlet pressure value at the corresponding position where the gas film thickness becomes lower are obtained to obtain a set of orifice outlet pressure values that satisfy the torque convergence condition and meet the thickness requirements.

上述步骤三中,调节节流孔出口压力使其满足力矩收敛条件,当所得一组数据满足力矩收敛要求而不满足承载力收敛要求时,可根据承载力偏小或偏大,对每个节流孔出口压力值同加或同减来改变承载力,再返回重新调节力矩收敛,以此往复,可到一组节流孔出口压力值,使力矩,承载力都满足收敛。 In the above step 3, the outlet pressure of the orifice is adjusted to meet the torque convergence condition. When the obtained set of data meets the torque convergence requirement but not the bearing capacity convergence requirement, the The orifice outlet pressure value is added or subtracted to change the bearing capacity, and then return to readjust the torque convergence, and so forth, to a set of orifice outlet pressure values, so that the torque and bearing capacity meet the convergence.

上述增大或减少出口压力值时,针对每个节流孔选用不相等的步长,即把每个节流孔出口压力的步长按各自相应位置气膜厚度变化大小的比例关系进行给定。 When increasing or decreasing the outlet pressure value above, choose an unequal step size for each orifice, that is, the step size of the outlet pressure of each orifice is given according to the proportional relationship between the change of the gas film thickness at the corresponding position .

上述步骤二中,不要求导轨调至等间隙后气膜厚度为偏载状态下受力斜面中心点厚度时,即气膜厚度初始值可高于或低于原倾斜承载面中心点厚度的值,在步骤三中同时调整所有节流孔出口压力值,或只调节部分节流孔位置相应气膜厚度增大幅度较多的节流孔出口压力来满足力矩的收敛条件。 In the above step 2, it is not required that the thickness of the gas film after the guide rail is adjusted to equal clearance is the thickness of the center point of the stressed slope under the partial load state, that is, the initial value of the gas film thickness can be higher or lower than the value of the center point thickness of the original inclined bearing surface , in step 3, adjust the outlet pressure values of all orifices at the same time, or only adjust the outlet pressure of the orifice with a larger increase in the corresponding gas film thickness at some orifice positions to meet the convergence condition of the torque.

上述步骤三中,同时调整所有节流孔出口压力值时,具体方法是先调节节流孔出口压力使其满足力矩收敛条件,所得一组数据不满足承载力收敛要求时,对气膜厚度进行小步长调整,改变承载力,再返回重新调节力矩收敛,以此往复,可得到一组节流孔出口压力值,使力矩,承载力都满足收敛。 In the above step 3, when adjusting the outlet pressure values of all orifices at the same time, the specific method is to first adjust the outlet pressure of the orifice to meet the torque convergence condition. Small step adjustment, change the bearing capacity, and then return to readjust the torque convergence, in this way, a set of orifice outlet pressure values can be obtained, so that the torque and bearing capacity meet the convergence.

与现有技术相比,本发明的优点是:利用本发明方法,和导轨垂直方向上产生的运动误差在理论上讲是没有的,即使因加工原因,也仅会产生极小的误差,相对于现有技术而言,本发明运行精度高,稳定性好。 Compared with the prior art, the advantages of the present invention are: using the method of the present invention, there is no movement error generated in the vertical direction of the guide rail in theory, and even due to processing reasons, only a very small error will be produced, relatively Compared with the prior art, the present invention has high operating precision and good stability.

附图说明 Description of drawings

图1为整体式气浮导轨非等间隙状态一个偏载受力面示意图; Figure 1 is a schematic diagram of an eccentric load bearing surface of the integral air bearing guide rail in the non-equal gap state;

图2为经过调整后得到的等间隙气浮导轨受力面示意图。 Figure 2 is a schematic diagram of the force-bearing surface of the equal-gap air-floating guide rail obtained after adjustment.

具体实施方式 Detailed ways

现有技术中,整体式气浮导轨承受偏载后,将导致导轨间隙不相等,进而影响工作精度。由于气膜厚度很小,很小的偏角就有可能引起刮蹭,影响轴承稳定性。本发明的原理如下:如果能对导轨加一个预偏角,使得工作过程中导轨的偏载产生的偏角与之抵消,从而恢复平行即等间隙状态,就可以提高稳定性以及工作精度。整体式气浮导轨的等间隙设计原理是以整体式气浮导轨的等间隙为目标, 在雷诺方程的控制下,通过质量守恒原理,找到一组实现目标满足约束的节流孔直径。 In the prior art, after the integral air-floating guide rail bears an eccentric load, the gap between the guide rails will be unequal, thereby affecting the working accuracy. Due to the small thickness of the air film, a small deflection angle may cause scratches and affect the stability of the bearing. The principle of the present invention is as follows: if a pre-deflection angle can be added to the guide rail, the deflection angle generated by the eccentric load of the guide rail during the working process can be offset to restore the parallel or equal gap state, and the stability and working accuracy can be improved. The equal clearance design principle of the integral air bearing guideway is to aim at the equal clearance of the integral air bearing guideway. Under the control of the Reynolds equation and through the principle of mass conservation, find a set of orifice diameters that meet the target and meet the constraints.

下面将结合附图和实施例对本发明进行详细地说明。 The present invention will be described in detail below with reference to the drawings and embodiments.

实施例1:整体式气浮导轨在偏载下的等间隙设计方法,包括下述步骤: Embodiment 1: The design method of the equal clearance of the integral air-floating guide rail under partial load, including the following steps:

步骤一: step one:

8节流孔整体式气浮导轨受偏载时会产生如图1所示的一个偏角,可将气浮导轨偏载简化为斜面中心点的合力F,以及两个坐标的偏载力矩Mx,My。图中n1,n2为两个斜面的法线,夹角为,即为本文中要讨论到的偏角。由图可见,外载垂直于斜面,而非竖直向下。故而可将F分解为水平力和竖直力Fz的合力。而水平力不会在此产生偏载,因而,要抵消偏载使导轨变回水平,可只讨论竖直力Fz。由静力学可知,气膜压力提供的承载力应该等于Fz。而气体压力对X轴,Y轴的总力矩应分别等于Mx,My。利用气体质量守恒原理确定的连续条件,将X,Y平面按8个节流孔位置划分为8个区域,通过将8个区域进出气体流量平衡进行嵌套耦合,可算出偏载时各节流孔出口压力,通过雷诺方程可得到偏载时的压力分布。积分可得到Fz,Mx,My。 When the 8-throttle integrated air bearing guide rail is subjected to an eccentric load, it will produce a deflection angle as shown in Figure 1. The eccentric load of the air bearing guide rail can be simplified as the resultant force F of the center point of the inclined plane, and the eccentric load moment Mx of the two coordinates , My. In the figure, n1 and n2 are the normals of the two slopes, and the included angle is , which is the declination angle to be discussed in this article. It can be seen from the figure that the external load is perpendicular to the slope, not vertically downward. Therefore, F can be decomposed into the resultant force of horizontal force and vertical force Fz. The horizontal force will not produce an eccentric load here, therefore, to offset the eccentric load and make the guide rail return to the level, only the vertical force Fz can be discussed. It can be seen from statics that the bearing capacity provided by the air film pressure should be equal to Fz. And the total torque of the gas pressure on the X-axis and the Y-axis should be equal to Mx and My respectively. Using the continuous condition determined by the principle of gas mass conservation, the X and Y planes are divided into 8 areas according to the positions of 8 orifices. By nesting and coupling the flow balance of the gas in and out of the 8 areas, the throttling under partial load can be calculated. The outlet pressure of the hole can be obtained by the Reynolds equation to obtain the pressure distribution under eccentric load. Points can get Fz, Mx, My.

步骤二: Step two:

当要求气浮导轨调至等间隙后气膜厚度为偏载状态下长导轨中心点厚度时,则令等间隙调平后均为此厚度见图2。将此厚度作为常量应用在雷诺方程中,以有偏角时得到的各节流孔出口压力值赋予等间隙调平后相应的节流孔出口压力计算此时的气体压力分布,通过积分计算此时气膜承载力F1与偏载力矩Mx1,My1。 When it is required that the air film thickness of the air-floating guide rail is adjusted to the equal clearance to be the thickness of the center point of the long guide rail under the eccentric load state, then the thickness is the same after the equal clearance is adjusted, as shown in Figure 2. Apply this thickness as a constant in the Reynolds equation, assign the outlet pressure value of each orifice obtained when there is a deflection angle to the corresponding orifice outlet pressure after equal clearance and leveling to calculate the gas pressure distribution at this time, and calculate this by integral When air film bearing capacity F1 and eccentric load moment Mx1, My1.

步骤三: Step three:

由于等间隙调平后,除平面中心点厚度没变以外,其余位置气膜厚度都有变化,必将导致压力分布的变化。此时的F1、Mx1、My1,必不与非等间隙状态下的Fz、Mx、My相等。此时,可根据各节流孔位置处气膜厚度的变化大小,分别给予各节流孔不等的步长,同时调整各节流孔出口压力大小。即增大相应位置气膜厚度变高的节流孔出口压力,减小相应位置气膜厚度变低的节流孔出口压力。从而达到两个力矩Mx1、My1,与非等间隙时两个力矩Mx、My相等的收敛条件。 After equal clearance leveling, except for the thickness of the center point of the plane, the thickness of the gas film at other positions changes, which will inevitably lead to changes in the pressure distribution. At this time, F1, Mx1, and My1 must not be equal to Fz, Mx, and My in the non-equal gap state. At this time, different step lengths can be given to each orifice according to the variation of the gas film thickness at the position of each orifice, and the outlet pressure of each orifice can be adjusted at the same time. That is, increase the outlet pressure of the orifice where the gas film thickness at the corresponding position becomes higher, and decrease the outlet pressure of the orifice where the gas film thickness becomes lower at the corresponding position. Thus the convergence condition that the two moments Mx1, My1 are equal to the two moments Mx, My when the gap is not equal is achieved.

根据此时得到的节流孔出口压力计算F1,以F1与Fz相等为收敛条件,将其与Fz进行对比,若F1小于Fz,则以相等的步长同时增加8个节流孔出口压力,来增大F1;若F1大于Fz,则以相等的步长同时减小8个节流孔出口压力,再以增加后的出口压力来计算Mx1、My1,并重新调节节流孔出口压力使Mx1、My1达到收敛条件,以此循环往复,最终经过调整得到一组使Mx1、My1、F1都能满足收敛条件的节流孔出口压力值。 Calculate F1 based on the orifice outlet pressure obtained at this time, and compare it with Fz under the condition that F1 and Fz are equal. If F1 is less than Fz, increase the outlet pressure of 8 orifices at the same time with equal steps. to increase F1; if F1 is greater than Fz, reduce the outlet pressure of 8 orifices at the same time with equal steps, and then calculate Mx1 and My1 with the increased outlet pressure, and readjust the outlet pressure of the orifice to make Mx1 , My1 reach the convergence condition, repeat this cycle, and finally obtain a set of orifice outlet pressure values that make Mx1, My1, and F1 all meet the convergence condition after adjustment.

步骤四: Step four:

步骤三得到的8个节流孔出口压力值通过雷诺方程可得到此时的压力分布。选取原节流孔内径值为调平后节流孔内径初始值,将XY平面按节流孔个数分为8个区域,以保证每个区域只有一个节流孔,再以每个区域气体进出气体流量相等为收敛条件,调节各个节流孔内径。即如果区域进入流量大于流出流量,则以小步长减小内径值;若进入流量小于流出流量,则以小步长增加内径值,直到进出气体流量相等为止。这样就得到一组节流孔内径值,能满足气膜厚度等间隙调平后,承载力和偏载力矩与非等间隙状态下相等。 The outlet pressure values of the 8 orifices obtained in Step 3 can be used to obtain the pressure distribution at this time through the Reynolds equation. Select the inner diameter of the original orifice as the initial value of the inner diameter of the orifice after leveling, divide the XY plane into 8 areas according to the number of orifices, to ensure that each area has only one orifice, and then use the gas in each area The inflow and outflow gas flow is equal to the convergence condition, and the inner diameter of each orifice is adjusted. That is, if the inflow flow rate of the area is greater than the outflow flow rate, the inner diameter value will be reduced in small steps; if the inflow flow rate is smaller than the outflow flow rate, the inner diameter value will be increased in a small step size until the inflow and outflow gas flow rates are equal. In this way, a set of inner diameter values of the orifice can be obtained, which can satisfy the equal clearance of the air film thickness.

实施例2,整体式气浮导轨在偏载下的等间隙设计方法,包括下述步骤: Embodiment 2, the equal clearance design method of the integral air-floating guide rail under partial load, includes the following steps:

步骤一: step one:

8节流孔整体式气浮导轨受偏载时会产生一个偏角,可将气浮导轨偏载简化为斜面中心点的合力F,以及两个坐标的偏载力矩Mx,My。图中n1,n2为两个斜面的法线,夹角为,即为本文中要讨论到的偏角。由图可见,外载垂直于斜面,而非竖直向下。故而可将F分解为水平力和竖直力Fz的合力。而水平力不会在此产生偏载,因而,要抵消偏载使导轨变回水平,可只讨论竖直力Fz。由静力学可知,气膜压力提供的承载力应该等于Fz。而气体压力对X轴,Y轴的总力矩应分别等于Mx,My。利用气体质量守恒原理确定的连续条件,将X,Y平面按8个节流孔位置划分为8个区域,通过将8个区域进出气体流量平衡进行嵌套耦合,可算出偏载时各节流孔出口压力,通过雷诺方程可得到偏载时的压力分布,积分可得到Fz,Mx,My。 When the 8-throttle integrated air bearing guide rail is subjected to an eccentric load, it will produce a deflection angle, which can simplify the eccentric load of the air bearing guide rail to the resultant force F of the center point of the inclined plane, and the eccentric load moments Mx, My of the two coordinates. In the figure, n1 and n2 are the normals of the two slopes, and the included angle is , which is the declination angle to be discussed in this article. It can be seen from the figure that the external load is perpendicular to the slope, not vertically downward. Therefore, F can be decomposed into the resultant force of horizontal force and vertical force Fz. The horizontal force will not produce an eccentric load here, therefore, to offset the eccentric load and make the guide rail return to the level, only the vertical force Fz can be discussed. It can be seen from statics that the bearing capacity provided by the air film pressure should be equal to Fz. And the total torque of the gas pressure on the X-axis and the Y-axis should be equal to Mx and My respectively. Using the continuous condition determined by the principle of gas mass conservation, the X and Y planes are divided into 8 areas according to the positions of 8 orifices. By nesting and coupling the flow balance of the gas in and out of the 8 areas, the throttling under partial load can be calculated. The outlet pressure of the hole can be obtained by the Reynolds equation when the pressure distribution is eccentrically loaded, and the integral can be used to obtain Fz, Mx, My.

步骤二: Step two:

当不要求气浮导轨调至等间隙后,气膜厚度为偏载状态下长导轨中心点厚度时,即气膜厚度初始值可高于或低于原倾斜承载面中心点厚度的值。将此厚度作为常量应用在雷诺方程中,以有偏角时得到的各节流孔出口压力值赋予等间隙调平后相应的节流孔出口压力计算此时的气体压力分布,通过积分计算此时气膜承载力F1与偏载力矩Mx1,My1。 When the air bearing guide rail is not required to be adjusted to equal clearance, the thickness of the air film is the thickness of the center point of the long guide rail under the partial load state, that is, the initial value of the air film thickness can be higher or lower than the value of the center point thickness of the original inclined bearing surface. Apply this thickness as a constant in the Reynolds equation, assign the outlet pressure value of each orifice obtained when there is a deflection angle to the corresponding orifice outlet pressure after equal clearance and leveling to calculate the gas pressure distribution at this time, and calculate this by integral When air film bearing capacity F1 and eccentric load moment Mx1, My1.

步骤三: Step three:

由于等间隙调平后,除平面中心点厚度没变以外,其余位置气膜厚度都有变化,必将导致压力分布的变化。此时的F1、Mx1、My1,必不与非等间隙状态下的Fz、Mx、My相等。此时,可根据各节流孔位置处气膜厚度的变化大小,分别给予各节流孔不等的步长,同时调整各节流孔出口压力大小。即增大相应位置气膜厚度变高的节流孔出口压力,减小相应位置气膜厚度变低的节流孔出口压力。从而达到两个力矩Mx1、My1,与非等间隙时两个力矩Mx、My相等的收敛条件。 After equal clearance leveling, except for the thickness of the center point of the plane, the thickness of the gas film at other positions changes, which will inevitably lead to changes in the pressure distribution. At this time, F1, Mx1, and My1 must not be equal to Fz, Mx, and My in the non-equal gap state. At this time, different step lengths can be given to each orifice according to the variation of the gas film thickness at the position of each orifice, and the outlet pressure of each orifice can be adjusted at the same time. That is, increase the outlet pressure of the orifice where the gas film thickness at the corresponding position becomes higher, and decrease the outlet pressure of the orifice where the gas film thickness becomes lower at the corresponding position. Thus the convergence condition that the two moments Mx1, My1 are equal to the two moments Mx, My when the gap is not equal is achieved.

根据此时得到的节流孔出口压力计算F1,以F1与Fz相等为收敛条件,将其与Fz进行对比,若F1小于Fz,则以相等的步长同时增加8个节流孔出口压力,来增大F1;若F1大于Fz,则以相等的步长同时减小8个节流孔出口压力,再以增加后的出口压力来计算Mx1、My1,并重新调节节流孔出口压力使Mx1、My1达到收敛条件,以此循环往复,最终经过调整得到一组使Mx1、My1、F1都能满足收敛条件的节流孔出口压力值。 Calculate F1 based on the orifice outlet pressure obtained at this time, and compare it with Fz under the condition that F1 and Fz are equal. If F1 is less than Fz, increase the outlet pressure of 8 orifices at the same time with equal steps. to increase F1; if F1 is greater than Fz, reduce the outlet pressure of 8 orifices at the same time with equal steps, and then calculate Mx1 and My1 with the increased outlet pressure, and readjust the outlet pressure of the orifice to make Mx1 , My1 reach the convergence condition, repeat this cycle, and finally obtain a set of orifice outlet pressure values that make Mx1, My1, and F1 all meet the convergence condition after adjustment.

步骤四: Step four:

步骤三得到的8个节流孔出口压力值通过雷诺方程可得到此时的压力分布。选取原节流孔内径值为调平后节流孔内径初始值,将XY平面按节流孔个数分为8个区域,以保证每个区域只有一个节流孔,再以每个区域气体进出气体流量相等为收敛条件,调节各个节流孔内径。即如果区域进入流量大于流出流量,则以小步长减小内径值;若进入流量小于流出流量,则以小步长增加内径值,直到进出气体流量相等为止。这样就得到一组节流孔内径值,能满足气膜厚度等间隙调平后,承载力和偏载力矩与非等间隙状态下相等。 The outlet pressure values of the 8 orifices obtained in Step 3 can be used to obtain the pressure distribution at this time through the Reynolds equation. Select the inner diameter of the original orifice as the initial value of the inner diameter of the orifice after leveling, and divide the XY plane into 8 areas according to the number of orifices to ensure that each area has only one orifice. The inflow and outflow gas flow is equal to the convergence condition, and the inner diameter of each orifice is adjusted. That is, if the inflow flow rate of the area is greater than the outflow flow rate, then reduce the inner diameter value in small steps; if the inflow flow rate is smaller than the outflow flow rate, increase the inner diameter value in small step sizes until the inflow and outflow gas flow rates are equal. In this way, a set of inner diameter values of the orifice can be obtained, which can satisfy the equal clearance of the air film thickness.

实施例3: Example 3:

整体式气浮导轨在偏载下的等间隙设计方法,其特征在于以下步骤: The equal-gap design method of integral air-floating guide rail under partial load is characterized by the following steps:

  一、以长导轨平面为XY坐标平面计算气浮导轨偏载状态下的各个节流孔出口压力,气膜承载力,以及气膜气体压力对X轴与对Y轴的力矩大小; 1. Taking the plane of the long guide rail as the XY coordinate plane to calculate the outlet pressure of each orifice of the air-floating guide rail under the eccentric load state, the bearing capacity of the gas film, and the moment of the gas pressure of the gas film to the X-axis and to the Y-axis;

二、利用雷诺方程以及重积分,计算等间隙状态下气膜承载力和气体对X轴与对Y轴的力矩大小:不要求导轨调至等间隙后气膜厚度为偏载状态下受力斜面中心点厚度时,即气膜厚度初始值可高于或低于原倾斜承载面中心点厚度的值; 2. Using the Reynolds equation and heavy integrals, calculate the bearing capacity of the air film and the moment of the gas on the X-axis and Y-axis in the state of equal clearance: it is not required that the thickness of the air film after the guide rail is adjusted to the equal clearance is the force slope under the partial load state When the center point thickness is used, that is, the initial value of the air film thickness can be higher or lower than the value of the center point thickness of the original inclined bearing surface;

三、以等间隙状态下气膜承载力和偏载力矩与非等间隙状态下都相等为收敛条件,调整节流孔出口压力,得到满足收敛条件的一组节流孔出口压力值:同时调整所有节流孔出口压力值,来满足力矩的收敛条件,同时调整的具体方法是先调节节流孔出口压力使其满足力矩收敛条件,所得一组数据不满足承载力收敛要求时,对气膜厚度进行小步长调整,改变承载力,再返回重新调节力矩收敛,以此往复,可得到一组节流孔出口压力值,使力矩、承载力都满足收敛; 3. Taking the air film bearing capacity and eccentric load moment in the equal clearance state as the convergence condition as the non-equal clearance state, adjust the outlet pressure of the orifice to obtain a set of orifice outlet pressure values that meet the convergence conditions: adjust at the same time The outlet pressure values of all orifices meet the convergence conditions of the torque. The specific method of adjustment at the same time is to adjust the outlet pressure of the orifices to meet the convergence conditions of the torque. When a set of data obtained does not meet the convergence requirements of the bearing capacity, the Adjust the thickness in small steps, change the bearing capacity, and then return to readjust the torque convergence, and reciprocate in this way, a set of orifice outlet pressure values can be obtained, so that the torque and bearing capacity meet the convergence;

四、选取原节流孔内径值为调平后节流孔内径初始值,将XY平面按节流孔个数分为多个区域,分别利用气体流量守恒方程进行嵌套耦合,即以满足各区域进出气体流量相等同时满足整个气膜总进出气体流量相等为收敛条件,若计算过程中某个区域进出气体流量不守恒,则以小步长调节节流孔内径值,直到满足收敛条件。 4. Select the inner diameter of the original orifice as the initial value of the inner diameter of the orifice after leveling, divide the XY plane into multiple areas according to the number of orifices, and use the gas flow conservation equation to perform nested coupling respectively, that is, to satisfy each The convergence condition is that the gas flow in and out of the area is equal and the total gas flow in and out of the entire gas film is equal. If the gas flow in and out of a certain area is not conserved during the calculation process, the inner diameter of the orifice is adjusted in small steps until the convergence condition is met.

实施例4: Example 4:

整体式气浮导轨在偏载下的等间隙设计方法,其特征在于以下步骤: The equal-gap design method of integral air-floating guide rail under partial load is characterized by the following steps:

    一、以长导轨平面为XY坐标平面计算气浮导轨偏载状态下的各个节流孔出口压力,气膜承载力,以及气膜气体压力对X轴与对Y轴的力矩大小; 1. Taking the plane of the long guide rail as the XY coordinate plane to calculate the outlet pressure of each orifice of the air-floating guide rail under the eccentric load state, the bearing capacity of the gas film, and the moment of the gas pressure of the gas film to the X-axis and to the Y-axis;

二、利用雷诺方程以及重积分,计算等间隙状态下气膜承载力和气体对X轴与对Y轴的力矩大小:不要求导轨调至等间隙后气膜厚度为偏载状态下受力斜面中心点厚度时,即气膜厚度初始值可高于或低于原倾斜承载面中心点厚度的值; 2. Using the Reynolds equation and heavy integrals, calculate the bearing capacity of the air film and the moment of the gas on the X-axis and Y-axis in the state of equal clearance: it is not required that the thickness of the air film after the guide rail is adjusted to the equal clearance is the force slope under the partial load state When the center point thickness is used, that is, the initial value of the air film thickness can be higher or lower than the value of the center point thickness of the original inclined bearing surface;

三、以等间隙状态下气膜承载力和偏载力矩与非等间隙状态下都相等为收敛条件,调整节流孔出口压力,得到满足收敛条件的一组节流孔出口压力值:只调节部分节流孔位置相应气膜厚度增大幅度较多的节流孔出口压力来满足力矩的收敛条件,所得一组数据不满足承载力收敛要求时,对气膜厚度进行小步长调整,改变承载力,再返回重新调节力矩收敛,以此往复,可得到一组节流孔出口压力值,使力矩、承载力都满足收敛; 3. Taking the air film bearing capacity and eccentric load moment in the equal clearance state as the convergence condition as the non-equal clearance state, adjust the outlet pressure of the orifice to obtain a set of orifice outlet pressure values that meet the convergence conditions: only adjust Part of the orifice position corresponding to the gas film thickness increases a lot to meet the convergence condition of the torque. When a set of data obtained does not meet the bearing capacity convergence requirements, the gas film thickness is adjusted in small steps, changing Bearing capacity, and then return to readjust the torque convergence, and reciprocate in this way, a set of orifice outlet pressure values can be obtained, so that the torque and bearing capacity meet the convergence;

四、选取原节流孔内径值为调平后节流孔内径初始值,将XY平面按节流孔个数分为多个区域,分别利用气体流量守恒方程进行嵌套耦合,即以满足各区域进出气体流量相等同时满足整个气膜总进出气体流量相等为收敛条件,若计算过程中某个区域进出气体流量不守恒,则以小步长调节节流孔内径值,直到满足收敛条件。 4. Select the inner diameter of the original orifice as the initial value of the inner diameter of the orifice after leveling, divide the XY plane into multiple areas according to the number of orifices, and use the gas flow conservation equation to perform nested coupling respectively, that is, to satisfy each The convergence condition is that the gas flow in and out of the area is equal and the total gas flow in and out of the entire gas film is equal. If the gas flow in and out of a certain area is not conserved during the calculation process, the inner diameter of the orifice is adjusted in small steps until the convergence condition is met.

Claims (6)

1.一种整体式气浮导轨在偏载下的等间隙设计方法,通过改变各节流孔内径大小来实现对导轨由于偏载带来的偏角进行调平,其特征在于以下步骤: 1. A method for equal clearance design of an integral air-floating guide rail under eccentric load, by changing the inner diameter of each orifice to achieve leveling the deflection angle of the guide rail due to eccentric load, characterized in the following steps:  一、以长导轨平面为XY坐标平面计算气浮导轨偏载状态下的各个节流孔出口压力,气膜承载力,以及气膜气体压力对X轴与对Y轴的力矩大小; 1. Taking the plane of the long guide rail as the XY coordinate plane to calculate the outlet pressure of each orifice of the air-floating guide rail under the partial load state, the bearing capacity of the gas film, and the moment of the gas pressure of the gas film to the X-axis and to the Y-axis; 二、利用雷诺方程以及重积分,计算等间隙状态下气膜承载力和气体对X轴与对Y轴的力矩大小; 2. Using the Reynolds equation and heavy integrals, calculate the gas film bearing capacity and the moment of gas on the X-axis and Y-axis under the equal gap state; 三、以等间隙状态下气膜承载力和偏载力矩与非等间隙状态下都相等为收敛条件,调整节流孔出口压力,得到满足收敛条件的一组节流孔出口压力值; 3. Taking the gas film bearing capacity and eccentric load moment in the equal clearance state as the convergence condition as the non-equal clearance state, adjust the orifice outlet pressure to obtain a set of orifice outlet pressure values that meet the convergence conditions; 四、则选取原节流孔内径值为调平后节流孔内径初始值,将XY平面按节流孔个数分为多个区域,分别利用气体流量守恒方程进行嵌套耦合,即以满足各区域进出气体流量相等同时满足整个气膜总进出气体流量相等为收敛条件,若计算过程中某个区域进出气体流量不守恒,则以小步长调节节流孔内径值,直到满足收敛条件。 4. The original orifice inner diameter is selected as the initial value of the orifice inner diameter after leveling, and the XY plane is divided into multiple regions according to the number of orifices, and the gas flow conservation equation is used for nested coupling, that is, to satisfy The convergence condition is that the gas flow in and out of each area is equal and the total gas flow in and out of the entire gas film is equal. If the gas flow in and out of a certain area is not conserved during the calculation process, the inner diameter of the orifice is adjusted in small steps until the convergence condition is met. 2.根据权利要求1所述的整体式气浮导轨在偏载下的等间隙设计方法,其特征在于:当所述步骤二中,要求导轨调至等间隙后气膜厚度为调整前受力斜面中心点厚度时,在所述步骤三中,对节流孔出口压力初始值进行调节时,同时增大相应位置气膜厚度变高的节流孔出口压力和减小对应位置气膜厚度变低的节流孔出口压力值,以得到满足力矩收敛条件同时满足厚度要求的一组节流孔出口压力值。 2. The design method for equal gaps of integral air-floating guide rails under eccentric loads according to claim 1, characterized in that: in the second step, the thickness of the air film after the guide rails are adjusted to equal gaps is required to be the force before adjustment When the thickness of the center point of the slope is thicker, in the step three, when adjusting the initial value of the orifice outlet pressure, increase the orifice outlet pressure at the corresponding position where the gas film thickness becomes higher and decrease the corresponding position where the gas film thickness becomes higher. A low orifice outlet pressure value is used to obtain a set of orifice outlet pressure values that satisfy the torque convergence conditions and meet the thickness requirements. 3.根据权利要求2所述的整体式气浮导轨在偏载下的等间隙设计方法,其特征在于:步骤三中,调节节流孔出口压力使其满足力矩收敛条件,当所得一组数据满足力矩收敛要求而不满足承载力收敛要求时,可根据承载力偏小或偏大,对每个节流孔出口压力值同加或同减来改变承载力,再返回重新调节力矩收敛,以此往复,可到一组节流孔出口压力值,使力矩,承载力都满足收敛。 3. The equal clearance design method of integral air-floating guide rail under eccentric load according to claim 2, characterized in that: in step 3, the outlet pressure of the orifice is adjusted so that it meets the torque convergence condition, when the obtained set of data When the torque convergence requirement is met but the bearing capacity convergence requirement is not satisfied, the bearing capacity can be changed by adding or subtracting the outlet pressure value of each orifice according to the smaller or larger bearing capacity, and then returning to readjust the torque convergence to This reciprocation can reach a set of pressure values at the outlet of the orifice, so that the torque and bearing capacity are all satisfied. 4.据权利要求2或3所述的整体式气浮导轨在偏载下的等间隙设计方法,其特征在于,在增大或减少出口压力值时,针对每个节流孔选用不相等的步长,即把每个节流孔出口压力的步长按各自相应位置气膜厚度变化大小的比例关系进行给定。 4. According to claim 2 or 3, the equal clearance design method of integral air bearing guide rail under eccentric load is characterized in that, when increasing or decreasing the outlet pressure value, unequal valves are selected for each orifice. The step size, that is, the step size of the outlet pressure of each orifice is given according to the proportional relationship between the change of the gas film thickness at each corresponding position. 5.根据权利要求1所述的整体式气浮导轨在偏载下的等间隙设计方法,其特征在于:当所述步骤二中,不要求导轨调至等间隙后气膜厚度为偏载状态下受力斜面中心点厚度时,即气膜厚度初始值可高于或低于原倾斜承载面中心点厚度的值,在步骤三中同时调整所有节流孔出口压力值,或只调节部分节流孔位置相应气膜厚度增大幅度较多的节流孔出口压力来满足力矩的收敛条件。 5. The method for designing the equal clearance of the integral air-floating guide rail under partial load according to claim 1, characterized in that: in the second step, the thickness of the air film after the guide rail is adjusted to the equal clearance is not required to be in the partial load state When the thickness of the center point of the lower stressed inclined surface, that is, the initial value of the air film thickness can be higher or lower than the value of the center point thickness of the original inclined bearing surface, in step 3, adjust the outlet pressure values of all orifices at the same time, or only adjust part of the throttle. The position of the orifice corresponds to the gas film thickness and the outlet pressure of the orifice increases more to meet the convergence condition of the moment. 6.根据权利要求5所述的整体式气浮导轨在偏载下的等间隙设计方法,其特征在于:步骤三中,同时调整所有节流孔出口压力值时,具体方法是先调节节流孔出口压力使其满足力矩收敛条件,所得一组数据不满足承载力收敛要求时,对气膜厚度进行小步长调整,改变承载力,再返回重新调节力矩收敛,以此往复,可得到一组节流孔出口压力值,使力矩,承载力都满足收敛。 6. The equal-gap design method of integral air-floating guide rail under eccentric load according to claim 5, characterized in that: in step 3, when adjusting the outlet pressure values of all orifices at the same time, the specific method is to first adjust the throttling The outlet pressure of the hole makes it meet the torque convergence condition. When the obtained set of data does not meet the load-bearing capacity convergence requirement, adjust the gas film thickness in small steps to change the load-bearing capacity, and then return to readjust the torque convergence. In this way, a Set the outlet pressure value of the orifice to make the moment and bearing capacity meet the convergence.
CN201310297492.0A 2013-07-16 2013-07-16 Integrated type air-float guide rail under unbalance loading etc. gap design method Expired - Fee Related CN103352917B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201310297492.0A CN103352917B (en) 2013-07-16 2013-07-16 Integrated type air-float guide rail under unbalance loading etc. gap design method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201310297492.0A CN103352917B (en) 2013-07-16 2013-07-16 Integrated type air-float guide rail under unbalance loading etc. gap design method

Publications (2)

Publication Number Publication Date
CN103352917A CN103352917A (en) 2013-10-16
CN103352917B true CN103352917B (en) 2015-08-19

Family

ID=49309319

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201310297492.0A Expired - Fee Related CN103352917B (en) 2013-07-16 2013-07-16 Integrated type air-float guide rail under unbalance loading etc. gap design method

Country Status (1)

Country Link
CN (1) CN103352917B (en)

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3750961T2 (en) * 1987-06-29 1995-08-10 Nippon Telegraph & Telephone Screw drive guide working with static pressure.
JP2008303913A (en) * 2007-06-05 2008-12-18 Shinkawa Ltd Static pressure guide device
JP4445528B2 (en) * 2007-07-11 2010-04-07 住友重機械工業株式会社 Hydrostatic bearing
JP2009144849A (en) * 2007-12-17 2009-07-02 Panasonic Corp Fluid bearing type rotating device and information recording / reproducing device including the same

Also Published As

Publication number Publication date
CN103352917A (en) 2013-10-16

Similar Documents

Publication Publication Date Title
Zha et al. Straightness error modeling and compensation for gantry type open hydrostatic guideways in grinding machine
CN104537141B (en) Railroad curve line design method based on " 6 two-part easement curves "
CN104551838B (en) A kind of combined type camber of spring compensation device
CN105202028A (en) Pressure-feed air bearing provided with elastic damping air chambers
CN104714478A (en) Heavy double-column vertical lathe cross beam gravity deformation prediction method based on finite difference method
CN103352917B (en) Integrated type air-float guide rail under unbalance loading etc. gap design method
CN105114459B (en) A kind of high precision high rigidity pneumato-static slideway based on optical material
CN104091021A (en) Method for calculating bearing capacity of oil pad when oil pad inclines
CN102207130A (en) Air static pressure thrust bearing
CN113987714B (en) Dynamic multi-field solution method and system for oil film of spherical flow distribution pair of plunger pump
CN105666165A (en) Machine tool sliding plate structure
CN114924478A (en) Special vehicle rapid vehicle display cooperative control method
CN101417393A (en) Air-bearing support workstation design method
CN106286579B (en) The thrust articulated bearing structure of load sensor
Xing et al. Directional migration of impacting droplets on hydrophobic-superhydrophobic boundary
CN107657089B (en) Chemical toughened glass finite element model establishing method considering residual stress
CN106696916B (en) A kind of approximant hydraulic leveling method
CN105179478B (en) A kind of Porous gas suspension support system applied to full physical simulation
CN112632827A (en) Method for calculating static characteristics of aerostatic bearing based on finite difference method
CN105303003B (en) A kind of optimization method for disk brake push rod position
TWM348658U (en) Hydrostatic linear slide track
CN102632398A (en) High-precision and high-rigidity closed type aerostatic guideway
CN100450702C (en) Method for manufacturing static pressure guide rail
CN117249167A (en) an air flotation device
CN106195006B (en) A kind of method of the optimal liquid resistance ratio of definite hydrostatic slideway

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20150819

Termination date: 20160716

CF01 Termination of patent right due to non-payment of annual fee