CN109227226A - Uniform-sliding method for residence time in optical element processing process - Google Patents
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Abstract
本发明公开了一种光学元件加工过程中驻留时间的匀滑方法,该方法通过引入一个时间扩散模型对常规计算得到的驻留时间分布进行扩散,从而实现驻留时间的匀滑处理。经过匀滑处理后的驻留时间与原驻留时间相比,在相邻离散点上的时间差值相对较小,从而实现相邻离散点间的平滑过渡,进而降低加工过程中抛光工具频繁加速、减速对机床稳定性造成的影响。本发明一种光学元件加工过程中驻留时间的匀滑方法不仅能通过时间扩散处理提高计算的收敛效果,还能通过对驻留时间的匀滑处理减小相邻离散点间驻留时间的跳变程度,有利于提高数控加工的稳定性,进而减少因抛光工具频繁抖动对元件引入的中、高频误差。
The invention discloses a method for levelling the residence time in the process of optical element processing. The method adopts a time diffusion model to spread the residence time distribution obtained by conventional calculation, so as to realize the levelling treatment of the residence time. Compared with the original residence time, the dwell time after leveling treatment has a relatively small time difference between adjacent discrete points, so as to achieve a smooth transition between adjacent discrete points and reduce the frequency of polishing tools during processing. The influence of acceleration and deceleration on the stability of the machine tool. The method for smoothing the residence time in the optical element processing process of the present invention can not only improve the convergence effect of the calculation through time diffusion processing, but also reduce the residence time between adjacent discrete points through the smoothing processing of the residence time. The degree of jumping is conducive to improving the stability of CNC machining, thereby reducing the medium and high frequency errors caused by the frequent shaking of the polishing tool.
Description
技术领域technical field
本发明属于光学元件的加工领域,具体涉及一种光学元件加工过程中驻留时间的匀滑方法。The invention belongs to the processing field of optical elements, and particularly relates to a method for levelling the residence time during the processing of optical elements.
背景技术Background technique
随着光学技术的飞速发展及其应用范围的不断扩拓,人们对光学元件的面形精度、表面粗糙度等技术指标提出了越来越高的要求,非球面、大相对口径、纳米精度成为了现代光学元件的发展趋势。为了有效提高光学元件表面加工质量和满足现代化高精度加工技术的需求,技术人员开始采用高精度数控加工机床进行光学元件的加工。在数控加工过程中,抛光工具在被加工元件表面形成一定的相对运动速度和压力,从而去除被加工元件表面的多余材料。由于数字化技术的引入,抛光工具在被加工元件表面的运动轨迹可近似看作是在各个离散点上的连续移动,在单位时间内,抛光工具在单个离散点上对被加工元件的去除量称为去除函数,而抛光工具在各个离散点上的停留时间即为驻留时间。因此,如何规划抛光工具在被加工元件表面的驻留时间分布是实现高精度数控加工的关键。With the rapid development of optical technology and the continuous expansion of its application range, people have put forward higher and higher requirements for technical indicators such as surface accuracy and surface roughness of optical components. The development trend of modern optical components. In order to effectively improve the surface processing quality of optical components and meet the needs of modern high-precision processing technology, technicians began to use high-precision CNC machining machines to process optical components. During the CNC machining process, the polishing tool forms a certain relative movement speed and pressure on the surface of the machined element, thereby removing excess material on the surface of the machined element. Due to the introduction of digital technology, the motion trajectory of the polishing tool on the surface of the workpiece to be processed can be approximately regarded as a continuous movement at each discrete point. For the removal function, the dwell time of the polishing tool at each discrete point is the dwell time. Therefore, how to plan the residence time distribution of the polishing tool on the surface of the machined component is the key to achieve high-precision CNC machining.
现有技术中,求解驻留时间的方法主要分为全局最优解法和局部最优解法:In the prior art, the method for solving the dwell time is mainly divided into a global optimal solution method and a local optimal solution method:
1、全局最优解法1. Global optimal solution
当去除函数和被加工元件的待去除量为已知时,可通过最小二乘法等经典算法计算得到一组最优的驻留时间分布使得加工后元件表面的面形残差最小,而这组最优的驻留时间分布即为全局最优解。但在实际的高精度加工中,该计算过程涉及的数据量和运算量十分巨大,导致难以求得全局最优解。When the removal function and the amount to be removed of the processed component are known, a set of optimal residence time distributions can be calculated by classical algorithms such as the least squares method to minimize the residual surface shape of the processed component surface. The optimal residence time distribution is the global optimal solution. However, in the actual high-precision machining, the amount of data and computation involved in the calculation process is very large, which makes it difficult to obtain the global optimal solution.
2、局部最优解法2. Local optimal solution
为了在有限时间内计算得到一组较优的驻留时间分布,使加工后元件表面的面形残差尽可能小,通常会采用按比例估算迭代法、脉冲迭代法等算法求解驻留时间,而这组驻留时间分布即为局部最优解。然而,这种方法主要适用于抛光工具在元件表面的去除函数呈圆对称分布的情况,在针对磁流变抛光机等去除函数为非圆对称分布的抛光设备时,该方法的计算收敛效果有待提高。In order to obtain a set of optimal dwell time distribution within a limited time, and to make the surface shape residual on the surface of the component as small as possible after machining, algorithms such as proportional estimation iteration method and pulse iteration method are usually used to solve the dwell time. This set of residence time distributions is the local optimal solution. However, this method is mainly suitable for the case that the removal function of the polishing tool on the surface of the element is distributed in a circular symmetry. When the removal function of the magnetorheological polishing machine is a polishing device with a non-circular symmetry distribution, the calculation convergence effect of this method needs to be improve.
然而,上述两种方法均未考虑驻留时间分布的匀滑问题;当相邻离散点间驻留时间变化量过大时,即驻留时间分布不够匀滑,抛光工具在运动过程中可能出现频繁加速、减速等现象,从而对机床稳定性造成的影响,进而在被加工元件表面留下运动痕迹。通常情况下,该运动痕迹的空间尺寸在数量级上与相邻离散点的间距相当,对应于中、高频面形误差。由于该面形误差是加工设备在加工过程中引入的,且中、高频面形误差修正是当前数控加工的技术难点,所以难以通过二次加工对其进行修正。However, neither of the above two methods considers the smoothness of the residence time distribution; when the variation of the residence time between adjacent discrete points is too large, that is, the residence time distribution is not smooth enough, and the polishing tool may appear during the movement process. Frequent acceleration, deceleration and other phenomena, which will affect the stability of the machine tool, and then leave movement marks on the surface of the machined component. Typically, the spatial size of this motion trace is comparable in magnitude to the spacing of adjacent discrete points, corresponding to mid- and high-frequency surface shape errors. Since the surface shape error is introduced by the processing equipment during the processing, and the correction of the medium and high frequency surface shape error is the technical difficulty of the current CNC machining, it is difficult to correct it through secondary processing.
发明内容SUMMARY OF THE INVENTION
本发明的目的是为了克服现有技术中所存在的不足,提供一种光学元件加工过程中驻留时间的匀滑方法,该方法通过引入一个时间扩散模型对局部最优解法在迭代过程中计算得到的驻留时间分布进行扩散,从而实现驻留时间的匀滑处理;并且继承了局部最优解法的优点,计算量远小于全局最优解法。The purpose of the present invention is to overcome the deficiencies in the prior art, and provide a method for levelling the residence time in the optical element processing process. The obtained residence time distribution is diffused, so as to realize the smoothing treatment of the residence time; and inherits the advantages of the local optimal solution method, and the calculation amount is much smaller than that of the global optimal solution method.
本发明采用的技术方案为:一种光学元件加工过程中驻留时间的匀滑方法,通过引入一个时间扩散模型对常规计算得到的驻留时间分布进行扩散,从而实现驻留时间的匀滑处理,其具体步骤是:The technical scheme adopted in the present invention is as follows: a method for levelling the residence time in the optical element processing process, by introducing a time diffusion model to spread the residence time distribution obtained by conventional calculation, so as to realize the levelling treatment of the residence time , the specific steps are:
步骤1:建立时间扩散模型D(x,y),其中心位置为D(x0,y0),且D(x,y)满足总量归一化要求:Step 1: Establish a time diffusion model D(x,y), the center of which is D(x 0 ,y 0 ), and D(x,y) meets the total normalization requirements:
∑i,jD(xi,yj)=1 (1)∑ i,j D(x i , y j )=1 (1)
其中D(xi,yj)表示时间扩散后(xi,yj)位置的相对时间变化率;针对任一时间量t,以其所在位置做为中心点(x0,y0),使用扩散模型D(x,y)对时间量t进行扩散,则t·D(xi,yj)表示时间扩散后(xi,yj)位置的时间量。where D(x i , y j ) represents the relative time rate of change of (x i , y j ) position after time diffusion; for any time amount t, its position is taken as the center point (x 0 , y 0 ), Using the diffusion model D(x,y) to spread the time amount t, then t·D(x i ,y j ) represents the time amount of the (x i ,y j ) position after the time diffusion.
步骤2:待加工元件的面形误差为M(x,y),抛光工具在单位时间内的去除函数为I(x,y),在迭代计算过程中,通过单次迭代求解得到的驻留时间为T1(x,y);在驻留时间T1(x,y)内,理论去除量与待加工元件的面形误差M(x,y)的差值即为计算残差E1(x,y),可表示为:Step 2: The surface shape error of the component to be processed is M(x,y), and the removal function of the polishing tool in unit time is I(x,y). The time is T 1 (x, y); within the dwell time T 1 (x, y), the difference between the theoretical removal amount and the surface error M(x, y) of the component to be processed is the calculated residual E 1 (x,y), which can be expressed as:
E1(x,y)=M(x,y)-T1(x,y)**I(x,y) (2)E 1 (x, y)=M(x, y)-T 1 (x, y)**I(x, y) (2)
式中,**表示卷积,T1(x,y)**I(x,y)表示在驻留时间T1(x,y)内,抛光工具对待加工元件的去除量;In the formula, ** represents convolution, T 1 (x,y)**I(x,y) represents the removal amount of the element to be processed by the polishing tool within the dwell time T 1 (x, y);
步骤3:针对T1(x,y)中的每一个离散坐标点(xi,yj),将时间扩散模型D(x,y)在X、Y方向上进行平移,使其中心位置(x0,y0)移动到(xi,yj),记为Dij(x,y):Step 3: For each discrete coordinate point (x i , y j ) in T 1 (x, y), translate the time diffusion model D(x, y) in the X and Y directions to make its center position ( x 0 ,y 0 ) moves to (x i ,y j ), denoted as Di ij (x,y):
Dij(x,y)=D(x-xi,y-yj) (3)D ij (x, y)=D(xx i , yy j ) (3)
随后,使用扩散函数Dij(x,y)对点T1(xi,yj)进行由点到面的扩散处理,从而得到扩散后的时间分布Kij(x,y):Then, the point T 1 (x i ,y j ) is diffused from point to surface using the diffusion function D ij (x,y) to obtain the diffused time distribution K ij (x,y):
Kij(x,y)=Dij(x,y)·T1(xi,yj) (4)K ij (x, y)=D ij (x, y)·T 1 (x i , y j ) (4)
由于Dij(x,y)同样满足公式(1)所示的总量归一化要求,因此有:Since D ij (x, y) also satisfies the total normalization requirement shown in formula (1), there are:
∑i,jKij(x,y)=T1(xi,yj) (5)∑ i,j K ij (x, y)=T 1 (x i , y j ) (5)
kij(x,y)**I(x,y)≈T1(xi,yj)·I(x,y) (6)k ij (x, y)**I(x, y)≈T 1 (x i , y j )·I(x, y) (6)
步骤4:按照步骤3可得到针对各个离散点(xi,yj)进行扩散处理后的时间分布Kij(x,y),则匀滑后的驻留时间分布T1’(x,y)可表示为:Step 4: According to step 3, the time distribution K ij (x, y) after diffusion processing for each discrete point (x i , y j ) can be obtained, then the residence time distribution T 1 '(x, y after leveling) ) can be expressed as:
T′1(x,y)=∑i,jKij(x,y) (7)T′ 1 (x, y)=∑ i, j K ij (x, y) (7)
且匀滑后的驻留时间分布T1’(x,y)对应的去除量,应与匀滑前的驻留时间分布T1(x,y)对应的去除量近似相等:And the removal amount corresponding to the residence time distribution T 1 '(x, y) after level slip should be approximately equal to the removal amount corresponding to the residence time distribution T 1 (x, y) before level slip:
T′1(x,y)**I(x,y)≈T1(x,y)**I(x,y) (8)T′ 1 (x, y)**I(x, y)≈T 1 (x, y)**I(x, y) (8)
步骤5:待加工面形误差M(x,y)与匀滑后的驻留时间分布T1’(x,y)对应的去除量之差,即为单次驻留时间匀滑处理后的计算残差E1’(x,y):Step 5: The difference between the surface shape error M(x, y) to be processed and the removal amount corresponding to the residence time distribution T 1 '(x, y) after level-slipping is the result of a single residence-time level-slipping process. Compute the residual E 1 '(x,y):
E′1(x,y)=M(x,y)-T′1(x,y)**I(x,y) (9)E' 1 (x, y)=M(x, y)-T' 1 (x, y)**I(x, y) (9)
步骤6:将计算残差E1’作为待加工面形M,重复步骤2到步骤5,进行迭代计算,直到第n次迭代计算完成后,对应的计算残差En’满足要求,从而得到匀滑处理后的总驻留时间分布T’(x,y):Step 6: Take the calculation residual E 1 ' as the surface shape M to be processed, repeat steps 2 to 5, and perform iterative calculation until the nth iteration calculation is completed, and the corresponding calculation residual E n ' meets the requirements, thereby obtaining: The total residence time distribution T'(x,y) after the smoothing treatment:
式中,n代表循环迭代的总次数;由此实现光学元件加工驻留时间的匀滑处理。In the formula, n represents the total number of loop iterations; thus, the smoothing process of the optical element processing dwell time is realized.
本发明与现有技术相比所具有的优点及有益的技术效果如下:Compared with the prior art, the advantages and beneficial technical effects of the present invention are as follows:
(1)、本发明所述的一种光学元件加工过程中驻留时间的匀滑方法,能对抛光工具在元件表面的去除函数为非圆对称的情况起到补偿效果,提高迭代计算的收敛效果。(1) The method for levelling the residence time in the optical element processing process of the present invention can compensate for the situation that the removal function of the polishing tool on the surface of the element is non-circular symmetric, and improve the convergence of the iterative calculation. Effect.
(2)、本发明所述的一种光学元件加工过程中驻留时间的匀滑方法,能在迭代计算过程中通过对驻留时间的匀滑处理,减小相邻离散点间驻留时间跳变程度,从而降低加工过程中抛光工具频繁加速、减速对机床稳定性造成的影响,进而减小加工过程中设备对被加工元件引入的中高频面形误差。(2) The method for levelling the residence time in the optical element processing process of the present invention can reduce the residence time between adjacent discrete points by means of levelling the residence time in the iterative calculation process. The degree of jump, thereby reducing the influence of frequent acceleration and deceleration of the polishing tool on the stability of the machine tool during the processing process, thereby reducing the medium and high frequency surface error introduced by the equipment to the processed components during the processing process.
附图说明Description of drawings
图1是实现本发明所述一种光学元件加工过程中驻留时间的匀滑方法的流程图;Fig. 1 is the flow chart that realizes the leveling method of dwell time in a kind of optical element processing process of the present invention;
图2是实施例中所用的去除函数分布和时间扩散模型,图2(a)是实施例中所用的去除函数分布,图2(b)是实施例中所用的时间扩散模型;Fig. 2 is the removal function distribution and time diffusion model used in the embodiment, Fig. 2 (a) is the removal function distribution used in the embodiment, Fig. 2 (b) is the time diffusion model used in the embodiment;
图3是实施例中初始的待加工面形误差;Fig. 3 is the initial surface shape error to be processed in the embodiment;
图4是实施例中计算残差的均方根值(RMS)随迭代次数的变化趋势图(其中实线是未使用本发明所述一种光学元件加工过程中驻留时间的匀滑方法时计算残差的均方根值(RMS)随迭代次数的变化规律,虚线是使用本发明所述一种光学元件加工过程中驻留时间的匀滑方法时计算残差的均方根值(RMS)随迭代次数的变化规律);4 is a graph showing the variation trend of the root mean square value (RMS) of the calculated residuals with the number of iterations in the embodiment (wherein the solid line is when the method for leveling the residence time in the optical element processing according to the present invention is not used) The variation law of the root mean square value (RMS) of the calculated residual with the number of iterations, the dotted line is the root mean square value (RMS) of the calculated residual when the method of the present invention is used for the level-slip method of the residence time in the optical element processing process. ) changes with the number of iterations);
图5是实施例中计算残差的对比图,其中图5(a)是未使用本发明所述一种光学元件加工过程中驻留时间的匀滑方法时的计算残差,图5(b)是使用本发明所述一种光学元件加工过程中驻留时间的匀滑方法时的计算残差;Fig. 5 is a comparison diagram of the calculated residuals in the embodiment, wherein Fig. 5(a) is the calculated residuals without using the method of level-slipping of the dwell time in the optical element processing process of the present invention, Fig. 5(b) ) is the calculated residual error when using the level-slip method of the residence time in the optical element processing process of the present invention;
图6是实施例中计算残差的功率谱密度(PSD)分布(其中实线是未使用本发明所述一种光学元件加工过程中驻留时间的匀滑方法时计算残差的功率谱密度(PSD)分布,虚线是使用本发明所述一种光学元件加工过程中驻留时间的匀滑方法时计算残差的功率谱密度(PSD)分布);6 is the power spectral density (PSD) distribution of the residual calculated in the embodiment (wherein the solid line is the power spectral density of the residual calculated without using the method of the present invention for the leveling of the residence time in the optical element processing process) (PSD) distribution, the dotted line is the power spectral density (PSD) distribution of the residual calculated when the method of the present invention is used for the method of leveling the residence time in the optical element processing process);
图7是实施例中通过迭代计算得到的驻留时间对比图,其中图7(a)是未使用本发明所述一种光学元件加工过程中驻留时间的匀滑方法时的驻留时间分布,图7(b)是使用本发明所述一种光学元件加工过程中驻留时间的匀滑方法时的驻留时间分布;FIG. 7 is a comparison diagram of the dwell time obtained by iterative calculation in the embodiment, wherein FIG. 7(a) is the dwell time distribution without using the method of the present invention for the level-smoothing of the dwell time in the optical element processing process. , Fig. 7(b) is the residence time distribution when using the method of level-smoothing the residence time in the optical element processing process of the present invention;
图8是实施例中驻留时间的功率谱密度(PSD)分布(其中实线是未使用本发明所述一种光学元件加工过程中驻留时间的匀滑方法时驻留时间的功率谱密度(PSD)分布,虚线是使用本发明所述一种光学元件加工过程中驻留时间的匀滑方法时驻留时间的功率谱密度(PSD)分布)。8 is the power spectral density (PSD) distribution of the dwell time in the embodiment (wherein the solid line is the power spectral density of the dwell time without using the method of the present invention for the leveling of the dwell time in the optical element processing process) (PSD) distribution, the dotted line is the power spectral density (PSD) distribution of the dwell time when using the method of the present invention for a method of skidding the dwell time during optical element processing.
具体实施方式Detailed ways
下面结合附图并用具体实施例对本发明作进一步详细说明,有必要指出的是所述实施例只是用于对本发明的进一步描述,而并不意味着是对本发明保护范围的任何限定。The present invention will be further described in detail below with reference to the accompanying drawings and specific embodiments. It is necessary to point out that the embodiments are only used to further describe the present invention, and are not intended to limit the protection scope of the present invention.
本发明提出的一种光学元件加工过程中驻留时间的匀滑方法,其实现流程如图1所示。A method for levelling the residence time in the optical element processing process proposed by the present invention, the realization flow of which is shown in FIG. 1 .
第一步,根据所使用的加工机床及加工设备对应的去除函数模型I(x,y),建立实现本发明一种光学元件加工过程中驻留时间的匀滑方法所使用的时间扩散模型D(x,y);The first step, according to the removal function model I(x, y) corresponding to the used processing machine tool and processing equipment, establish a time diffusion model D used to realize a method of leveling the residence time in the optical element processing process of the present invention. (x,y);
第二步,根据待加工面形M(x,y)和去除函数I(x,y),通过单次迭代求解得到驻留时间Tn(x,y);In the second step, according to the surface shape to be processed M(x,y) and the removal function I(x,y), the dwell time Tn( x ,y) is obtained through a single iterative solution;
第三步,使用时间扩散模型D(x,y)对驻留时间Tn(x,y)进行匀滑处理,得到匀滑后的驻留时间Tn’(x,y);The third step is to use the time diffusion model D(x, y) to perform a smoothing process on the residence time T n (x, y) to obtain the residence time T n '(x, y) after the smoothing;
第四步,由匀滑处理后的驻留时间Tn’(x,y)和待加工面形M(x,y),求解得到计算残差En’(x,y);The fourth step, from the residence time T n '(x, y) after the levelling treatment and the surface shape M(x, y) to be processed, the calculation residual E n '(x, y) is obtained by solving;
第五步,把计算残差En’(x,y)作为待加工面形M(x,y),重复第二步到第四步,进行迭代计算,直到第n次迭代计算完成后,计算残差En’(x,y)满足要求;The fifth step is to take the calculated residual E n '(x, y) as the surface shape M(x, y) to be processed, repeat the second to fourth steps, and perform iterative calculation until the nth iteration calculation is completed, Calculate the residual E n '(x, y) to meet the requirements;
第六步,将每次计算得到的驻留时间Tn’(x,y)累加得到匀滑后的总驻留时间T’(x,y),并进入后续加工环节。In the sixth step, the dwell time T n '(x, y) obtained by each calculation is accumulated to obtain the total dwell time T'(x, y) after level slip, and the subsequent processing step is entered.
实施例Example
本实施例以磁流变数控抛光机为加工设备,以直径为100mm的圆形平面镜为待加工元件,并结合图2到图7,对本发明的具体实施方式进行举例说明。在后续描述过程中,将本发明所述的一种光学元件加工过程中驻留时间的匀滑方法简称为匀滑方法。在常规情况下,磁流变抛光机的去除函数呈非圆对称分布,图2(a)为磁流变抛光头在x=0,y=0的坐标点上驻留3秒时的去除函数分布I(x,y)。本实施例以图2(a)所示去除函数分布关于x=0,y=0坐标点旋转180度后的形状分布作为时间扩散模型D(x,y),其分布形态如图2(b)所示;并对该时间扩散模型进行总量归一化处理,使其满足公式(1)。In this embodiment, a magnetorheological numerical control polishing machine is used as the processing equipment, and a circular plane mirror with a diameter of 100 mm is used as the element to be processed. In the following description process, the method of the present invention for the levelling of the residence time in the optical element processing process is simply referred to as the levelling method. Under normal circumstances, the removal function of the magnetorheological polishing machine is non-circularly symmetrical. Figure 2(a) shows the removal function of the magnetorheological polishing head when the magnetorheological polishing head resides at the coordinate point of x=0, y=0 for 3 seconds Distribution I(x,y). In this embodiment, the shape distribution of the removal function distribution shown in Fig. 2(a) rotated 180 degrees about the coordinate point of x=0, y=0 is used as the time diffusion model D(x, y), and its distribution shape is shown in Fig. 2(b) ); and normalize the total amount of the time diffusion model to make it satisfy formula (1).
图3是待加工元件初始的待加工面形误差M(x,y),其面形峰谷值(PV)为200.076nm,均方根值(RMS)为36.115nm。将待加工面形误差M(x,y)和去除函数I(x,y)代入公式(2),即可求解得到未使用时间匀滑方法时的驻留时间分布T1(x,y)和对应的计算残差E1(x,y)。针对上述驻留时间T1(x,y),使用图2(b)所示的时间扩散模型D(x,y)按照公式(3)~(8)对其进行匀滑处理,即可得到使用匀滑方法后的驻留时间分布T1’(x,y),并可由公式(9)计算得到使用匀滑方法后的计算残差E1’(x,y)。Figure 3 shows the initial surface shape error M(x, y) of the component to be processed, the surface shape peak-valley (PV) is 200.076nm, and the root mean square (RMS) is 36.115nm. Substituting the surface shape error M(x,y) and the removal function I(x,y) into formula (2), the residence time distribution T 1 (x, y) can be obtained when the time level slip method is not used. and the corresponding computed residual E 1 (x,y). For the above dwell time T 1 (x, y), use the time diffusion model D(x, y) shown in Fig. 2(b) to perform a smoothing process on it according to formulas (3) to (8) to obtain The residence time distribution T 1 '(x, y) after using the level slip method can be calculated from the formula (9) to obtain the calculated residual E 1 '(x, y) after using the level slip method.
当不使用匀滑方法时,将上述计算残差E1(x,y)作为待加工面形误差M(x,y),并代入循环进行迭代计算;当使用匀滑方法时,将上述计算残差E1’(x,y)作为待加工面形误差M(x,y),并代入循环进行迭代计算。When the level slip method is not used, the above calculation residual E 1 (x, y) is used as the surface shape error M(x, y) to be processed, and is substituted into the loop for iterative calculation; when the level slip method is used, the above calculation The residual E 1 '(x, y) is used as the surface shape error M(x, y) to be processed, and is substituted into the loop for iterative calculation.
图4给出了在20次迭代计算中,计算残差的均方根值(RMS)随迭代次数的变化规律;其中,实线是未使用匀滑方法时计算残差的均方根值(RMS)随迭代次数的变化规律,虚线是使用匀滑方法后计算残差的均方根值(RMS)随迭代次数的变化规律。从图4可以看出,计算残差的均方根值(RMS)随迭代次数的增加,呈现出逐渐减小的趋势,并且在使用匀滑方法后,计算残差的均方根值(RMS)的收敛速度和收敛效果均优于不使用匀滑方法的情况。当不使用匀滑方法时,第20次迭代计算完成后的计算残差E20(x,y)如图5(a)所示,对应的峰谷值(PV)为96.258nm,均方根值(RMS)为12.263nm;而使用匀滑方法后,第20次迭代计算完成后的计算残差E20’(x,y)如图5(b)所示,对应的峰谷值(PV)为86.432nm,均方根值(RMS)为7.835nm。与图5(a)相比,图5(b)对应的面形分布更加均匀、平缓,其峰谷值(PV)和均方根值(RMS)也更小,表明该匀滑方法能提高迭代计算的收敛效果,即使是抛光工具在元件表面的去除函数为非圆对称分布情况,也能在使用该匀滑方法后达到较好的收敛效果。图6所示,对比了不使用匀滑方法时的计算残差E20(x,y)和使用匀滑方法后的计算残差E20’(x,y)的功率谱密度(Power Spectral density,PSD)分布。功率谱密度(PSD)为本领域的公知内容,在此不做进一步讲述,其数值计算公式为:Figure 4 shows the variation law of the root mean square (RMS) of the calculated residuals with the number of iterations in 20 iterative calculations; the solid line is the RMS value of the residuals calculated when the level slip method is not used ( RMS) with the number of iterations, and the dotted line is the change rule of the root mean square (RMS) of the residual calculated after using the level slip method with the number of iterations. It can be seen from Figure 4 that the root mean square value (RMS) of the calculated residual shows a decreasing trend with the increase of the number of iterations, and after using the smoothing method, the root mean square value (RMS) of the residual calculated ), the convergence speed and the convergence effect are better than those without the use of the level-slip method. When the level-slip method is not used, the calculated residual E 20 (x, y) after the 20th iteration calculation is shown in Figure 5(a), and the corresponding peak-to-valley (PV) value is 96.258 nm, the root mean square value (RMS) is 12.263nm; after using the level slip method, the calculated residual E 20 '(x, y) after the 20th iteration calculation is shown in Figure 5(b), the corresponding peak-to-valley value (PV ) is 86.432 nm, and the root mean square (RMS) value is 7.835 nm. Compared with Fig. 5(a), the surface distribution corresponding to Fig. 5(b) is more uniform and gentle, and its peak-to-valley (PV) and root mean square (RMS) are also smaller, indicating that the levelling method can improve the The convergence effect of the iterative calculation, even if the removal function of the polishing tool on the surface of the element is a non-circular symmetrical distribution, a better convergence effect can be achieved after using the leveling method. As shown in Figure 6, the power spectral density of the calculated residual E 20 (x, y) without the use of the level slip method and the calculated residual error E 20 '(x, y) after the use of the level slip method are compared (Power Spectral density) , PSD) distribution. Power Spectral Density (PSD) is well known in the art, and will not be further described here. Its numerical calculation formula is:
式中,△x=L/N为采样间隔,L为采样长度,N为有效采样点数,M(n)为误差函数。从图6可以看出,与未使用匀滑方法时相比,在使用匀滑方法后,计算残差面形中,空间频率低于0.2mm-1的部分(通常对应于中、低频误差)均有所减少,进而表明该匀滑方法能提高加工设备在中、低频部分的加工效果。In the formula, Δx=L/N is the sampling interval, L is the sampling length, N is the number of valid sampling points, and M(n) is the error function. It can be seen from Figure 6 that, compared with the case where the crossfading method is not used, after using the crossfading method, the part of the spatial frequency lower than 0.2mm -1 (usually corresponding to the middle and low frequency errors) in the residual surface shape is calculated. are reduced, which further indicates that the levelling method can improve the processing effect of the processing equipment in the middle and low frequency parts.
图7所示,对比了不使用匀滑方法和使用了匀滑方法时求解到的驻留时间分布。其中,各离散点所对应的空间尺寸为0.0383mm2,即使用了512×512个离散点对边长为100mm的方形区域进行离散处理;图7(a)是不使用匀滑方法时,第20次迭代计算完成后得到的总驻留时间T(x,y)分布,T(x,y)满足其对应的峰谷值(PV)为0.107秒,均方根值(RMS)为0.013秒;7(b)是使用了时间匀滑方法后,第20次迭代计算完成后的总驻留时间T’(x,y)分布,T’(x,y)满足其对应的峰谷值(PV)为0.038秒,均方根值(RMS)为0.006秒。由此看出,与不使用匀滑方法时计算得到的驻留时间相比,使用匀滑方法计算得到的驻留时间在峰谷值(PV)和均方根值(RMS)方面均有所减小,其时间分布更加均匀、平缓。图8从功率谱密度的角度,对比了驻留时间T(x,y)和T’(x,y)在空间频率上的分布特性。从图8可以看出,与不使用匀滑方法时相比,在使用匀滑方法后的驻留时间分布中,空间频率高于0.05mm-1的部分(通常对应于中、高频误差)均有所减少;表明该匀滑方法能减小抛光工具在小尺寸空间内的频繁运动程度,从而在加工过程中,减少因抛光工具频繁抖动对元件引入的中、高频误差。Figure 7 shows a comparison of the residence time distributions solved for without and with the use of the levelling method. Among them, the space size corresponding to each discrete point is 0.0383mm 2 , that is, 512×512 discrete points are used to discretize a square area with a side length of 100mm; Fig. 7(a) is the first step when the leveling method is not used. The total residence time T(x,y) distribution obtained after 20 iterations is calculated, T(x,y) satisfies The corresponding peak-to-valley value (PV) is 0.107 seconds, and the root mean square value (RMS) is 0.013 seconds; 7(b) is the total dwell time T after the 20th iterative calculation after the time smoothing method is used. '(x,y) distribution, T'(x,y) satisfies It corresponds to a peak-to-valley (PV) value of 0.038 seconds and a root mean square value (RMS) of 0.006 seconds. From this, it can be seen that the dwell time calculated using the cross-fade method has a lower peak-to-valley (PV) and root mean square (RMS) value than the dwell time calculated without the use of the cross-fade method. decreases, the time distribution is more uniform and smooth. Figure 8 compares the distribution characteristics of dwell times T(x,y) and T'(x,y) over spatial frequencies from the perspective of power spectral density. It can be seen from Fig. 8 that, compared with when the cross-fading method is not used, in the dwell time distribution after using the cross-fading method, the part of the spatial frequency higher than 0.05mm -1 (usually corresponding to the mid- and high-frequency errors) It shows that the smoothing method can reduce the frequent movement of the polishing tool in the small space, thereby reducing the medium and high frequency errors caused by the frequent shaking of the polishing tool during the processing.
通过上述实施例,表明了本发明所述的一种光学元件加工过程中驻留时间的匀滑方法能提高驻留时间求解过程中迭代计算的收敛效果,提高加工设备对被加工元件表面中、低频误差的加工能力;此外,本发明所述的一种光学元件加工过程中驻留时间的匀滑方法,通过对驻留时间的匀滑处理,减小了相邻离散点间驻留时间的跳变程度,从而降低加工过程中抛光工具频繁加速、减速对机床稳定性造成的影响,进而减少因抛光工具频繁抖动对被加工元件引入的中、高频误差。Through the above-mentioned embodiments, it is shown that the method of the present invention for a method of levelling the residence time in the optical element processing process can improve the convergence effect of the iterative calculation in the process of solving the residence time, and improve the accuracy of the processing equipment on the surface of the processed element, The processing capability of low-frequency error; in addition, the method for levelling the residence time in the optical element processing process of the present invention reduces the variation of the residence time between adjacent discrete points through the levelling processing of the residence time. The degree of jumping, thereby reducing the influence of frequent acceleration and deceleration of the polishing tool on the stability of the machine tool during the processing process, thereby reducing the medium and high frequency errors introduced by the frequent shaking of the polishing tool to the processed components.
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CN115401531A (en) * | 2022-09-19 | 2022-11-29 | 天津津航技术物理研究所 | Method and system for determining residence time of conformal polishing tool |
CN117473802A (en) * | 2023-12-28 | 2024-01-30 | 中国科学院长春光学精密机械与物理研究所 | Method for rapidly solving polishing residence time of large-caliber optical element |
CN117473802B (en) * | 2023-12-28 | 2024-03-19 | 中国科学院长春光学精密机械与物理研究所 | Quick solution method for polishing residence time of large-aperture optical components |
CN118081494A (en) * | 2024-04-28 | 2024-05-28 | 中国科学院长春光学精密机械与物理研究所 | Magnetorheological polishing method based on optimal removal function selection |
CN118123694A (en) * | 2024-05-06 | 2024-06-04 | 中国科学院长春光学精密机械与物理研究所 | Processing capability evaluation method based on hybrid robot magneto-rheological optical processing equipment |
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