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Abstract

The micro-topographic quality of a product’s surface directly affects the performance of the virtual assembly. The computational precision of the fractal dimension has a significant effect on the accuracy of the virtual assembly model. To address the imprecision and large deviation of the calculation method under some conditions, a virtual product assembly surface modeling method is proposed in this article based on the root mean square of the area residuals. First, the fractal dimension of the surface is calculated using the regional residual root mean square (3R method). The feasibility of the 3R method is verified by comparing with the existing methods on isotropic and anisotropic surfaces. Second, the fractal dimension of a real part surface is obtained using the 3R method. According to the Weierstrass–Mandelbrot function, a partial surface model of the machined part is established. The surface contours, roughness, waviness, and flatness of the part are extracted by wavelet transform. Then, the digital surface model for virtual assembly with the same profile parameters is generated by reconstructing the surface contours of the actual parts. Finally, the method proposed by taking the virtual assembly of a VTM200/F5 turn-milling composite machining center guideway is verified in this article.

Keywords

Fractal dimension surface modeling regional residuals root mean square wavelet transform virtual assembly

Introduction

The virtual prototyping technology uses the advantages of a virtual environment in visualization and interactive exploration of virtual objects functionality to realize virtual assembly and analyze assembly performance. Its very important to verify the assembly properties and predict the assembly accuracy by constructing a micro-topography of the part in virtual assembly. Early research on surface modeling of virtual prototype models focused on semantic modeling.^1,2 Digital modeling technology has been used widely in recent years.³ The existing digital simulation methods based on fractal theory mainly involve the modeling of fractal functions,^4–6 the calculation method of fractal dimension,^7,8 the extraction of surface parameters, and so on.^9,10

In the area of fractal modeling, the Weierstrass–Mandelbrot function (W-M function) is one of the most commonly used models. The W-M function was initially used to characterize fractal curves.¹¹ To facilitate its application, Ausloos and Berman¹¹ introduced the W-M function into a three-dimensional (3-D) rectangular coordinate system. Since then, many scholars have done a lot of research and applied it to engineering. Qiu et al. proposed a surface topography modeling method based on a multiscale altitude field. The normalized fractal function is used to simulate the surface microstructure of parts.¹² Liao et al.¹³ proposed a method to determine the contact stiffness and contact force of a shrink-fit tool-holder joint based on Hertz contact and fractal geometry theory. Ma et al.¹⁴ characterized the rough surface by W-M fractal function to study the thermal contact conductance in vacuum environment.

In researching the calculation methods of surface fractal dimension, various traditional methods have been proposed such as the differential box counting (DBC) method,^15,16 the triangle prism area method (TPSA),^17,18 and the variation method (VM).^19,20 With the efforts of many scholars, many other methods have been derived from traditional methods, which can be divided into two-dimensional (2-D) and 3-D areas. Liu et al.²¹ proposed a two-stage method based on the power spectrum method and structural function method to improve the precision of a 2-D fractal dimension calculation. Zuo et al.²² proposed a 2-D root mean square (RMS) method to estimate the fractal dimension, and studied the relationships between surface roughness, fractal dimension and material hardness, elongation, spindle speed, and feed rate, respectively. As for the 3-D problems, Zuo et al.²³ proposed a 3D RMS method to calculate the dimensions of machined surfaces. Jing et al.²⁴ proposed the perimeter-volume method which combined the virtues of the DBC method and the Peleg blanket method to calculate the dimensions of $S i_{3} N_{4}$ ceramic parts.

Once the modeling is complete, the surface parameters need to be extracted to verify the correctness of the model. Wavelet analysis is an efficient tool for extracting the surface parameters. The height information of the part is taken as the input signal, and the surface parameters can be taken as the output. Moktadir and Sato²⁵ used wavelet transform to characterize the surface roughness of anisotropically etched silicon. Wang et al.²⁶ introduced a wavelet packet transform for surface roughness characterization and surface texture extraction. Tangjitsitcharoen et al.²⁷ proposed a method to predict the surface roughness during the ball-end milling process by utilizing the wavelet transform to monitor and decompose the dynamic cutting forces. Pang et al.²⁸ put forward an extraction and reconstruction method for arbitrary 2-D and 3-D frequency features in precision machined surfaces based on the combination of power spectrum density and continuous wavelet transform to analyze the potassium dihydrogen phosphate crystal surface topography.

The research described above has made progress in fractal theory and surface parameter extraction which has been applied to practical engineering problems like surface modeling of machined parts and material wear. Semantic modeling and digital simulation are common methods of virtual assembly modeling. In semantic modeling, assembly semantics focuses on macroscopic assembly properties by describing the constraint relationships between parts by assembly semanteme. In digital simulation, the 2-D method can only describe the surface of turning parts, and its applicability is relatively poor. In some cases, the 3-D calculation method has unstable calculation accuracy and large deviation. To this end, a product modeling method for virtual assembly based on the RMS of regional residuals (3R method) is proposed in this article.

First, according to the actual surface information, the fractal dimension is solved by using the 3R method proposed in this article. The W-M fractal surface is constructed according to the obtained fractal dimensions, and the real parts are simulated with the digital model. Second, wavelet transform is used to extract the contour components, including roughness, waviness, and flatness contour and the reconstructed components are then synthesized. A surface model with the same profile parameters as the actual part is obtained. Finally, the method is verified in a virtual assembly using the VTM-200/F5 turn-milling composite machining center.

The rest of the article is arranged as follows. The second section is an overview of the proposed approach. The details of the method are explained in section “Calculation of Fractal Dimension by the area residuals method.” In section “Case study,” an experiment that involves slide in a computer numerical control (CNC) tool is conducted. The final section presents the conclusions.

Overview of approach

Its necessary to present a brief introduction of the W-M function. Ausloos and Berman¹¹ derived the W-M function in Cartesian coordinates expressed as in equation (1)

\begin{matrix} z (x, y) = A \sqrt{\frac{\ln γ}{M}} \sum_{m = 1}^{M} \sum_{n = 0}^{n_{max}} γ^{(D - 3) n} \\ {\cos ϕ_{m, n} - \cos [\frac{2 π γ^{n} \sqrt{x^{2} + y^{2}}}{L} \cos [ϕ_{θ} - \frac{π m}{M}] + ϕ_{m, n}]} \end{matrix}

(1)

where $(x, y)$ represents the Cartesian coordinates of any point of the sample. $D$ is an independent fractal dimension representing the surface. $A$ is created to simplify the expression that is related to the scaling coefficient and $A = L (G / L)^{(D - 2)} (\ln γ / M)^{1 / 2}$ . $L$ is the maximum size in the direction of the sample coordinates, which means $L = max (L_{x}, L_{y})$ . $M$ represents the number of contour peaks formed by superposition on the surface of the final part. The phase $ϕ_{m, n}$ with random distribution in the range of $[0 ~ 2 π]$ is introduced to avoid the overlap of different surface frequencies. $n_{\max}$ is the maximum sampling number, which can be written as $int [\log (L / L_{s}) / \log γ]$ , where $L_{s}$ is the sampling step and $int [\cdot]$ denotes the rounding operator.

This article presents a method for modeling part surfaces for virtual assembly. The main ideas are as follows: calculating the fractal dimension $D$ of the surface of the actual machined part, and using the 3-D W-M function to simulate the surface of the actual machined part.

Fractal dimension $D$ is the foundation of fractal theory modeling which needs to be obtained before modeling. Based on the characteristics of a 3-D fractal surface, the 3R method is proposed to calculate the fractal dimension of real parts. To verify the feasibility of the proposed method, the $D$ of the anisotropic and isotropic surfaces is calculated by the 3R method. The traditional DBC method, VM method, TPSA method, and the recently proposed 3D-RMS method are selected to calculate the same surface for comparison.

The $D$ obtained by the 3R method is brought into equation (1) to simulate the surface of the parts, and the numerical model is used to simulate the actual parts. According to the characteristics of the W-M fractal surface, after the fractal dimension $D$ is obtained by 3R method, another independent scale parameter $G$ value has not been determined. To keep the surface parameters of the model, the $G$ -related parameter $A$ is set as 1 in equation (1). Then using the wavelet transform to realize surface reconstruction can release the $G$ -related information.

According to the different “wavelength” of each surface component, wavelet transform is used to separate each contour component. The surface of each component is reconstructed and integrated according to the design parameters. By this method, a surface model with the same contour parameters as the actual part surface is obtained.

Calculation of fractal dimension by the area residuals method

Surface modeling based on fractal theory

The W-M fractal function can be applied to the microsurface of the machined part of the simulator. Researches show that the W-M function can simulate the isotropic surfaces like electrical discharge machining (EDM), grinding, and the polishing parts, and the anisotropic surface like turning and milling parts.²³ However, it still has some shortcomings and limitations. For surfaces with larger dimensions and tolerances, the W-M function may appear to be a large amount of data, time-consuming, and error-prone. For the surface with too small precision, it is also easy to cause the relative error to be too big and not cost-effective. Most of these surfaces belong to simple geometric surfaces, and it is rarely used on freeform surfaces. That is why the W-M function was chosen as the basis of the modeling method in this article.

The W-M function is commonly used in the field of surface roughness modeling and satisfies the self-similarity of fractal geometry on the statistical level. The curve of the function is continuous but non-differentiable at any point. The 2-D W-M function can be expressed as¹¹

z (x) = \sum_{n = n_{min}}^{n_{max}} \frac{G^{D - 1} \cos 2 π γ^{n} x}{{γ^{(2 - D)}}^{n}}

(2)

where $z (x)$ denotes the height of the roughness at the point $x$ . $G$ is the independent fractal parameter that characterizes the roughness height. $γ$ denotes the constant fractal scale parameter.²⁹ $L$ is the length of the sample with the resolution of $s$ . $n_{min}$ and $n_{max}$ are the lowest and highest cut frequencies, which lead to $γ^{n min} = 1 / L$ and $γ^{n max} = 1 / s$ .

To apply the W-M function to a 3-D field, Ausloos and Berman¹¹ introduced binary parameters $(ρ, θ)$ to represent plane polar coordinates. Then the expression of the 3-D W-M function under the rectangular coordinate system is derived as in equation (1).

Fractal dimension calculation method based on the RMS of regional residuals

The unique advantage of the W-M function in describing geometric error modeling of part surfaces has been proved in a large number of studies. Different computing methods lead to different results of fractal dimension in practical applications. Therefore, the accuracy of the fractal dimension is very important to the final model.

There are two strategies for calculating the fractal dimension according to the different characteristics of the 3-D fractal surface. The first strategy is dimension reduction. Based on Mandelbrots study,⁷ the relationship between the 2-D dimension $D_{l}$ and the surface dimension $D$ is that $D_{l}$ equals $D - 1$ . When applied to isotropic surfaces, calculating the 2-D dimension in a certain direction along the section, the dimension of the surface equals the 2-D dimension plus 1. This can reduce the computational complexity according to the first strategy, but when the surface properties are unknown, the error of the calculation results will be large, which will affect the subsequent results, and cannot accurately reflect the surface properties. The other strategy is the global computing strategy. This strategy is oriented to the anisotropic surface, because the fractal dimension of the anisotropic surface is different in different directions, and the first strategy cannot satisfy the requirements of anisotropic surface calculation. Therefore, the second calculation strategy should be adopted on the premise that the surface properties are not completely clear. In this article, a fractal dimension calculation method based on the RMS of regional residuals (3R method) is used to calculate the fractal dimension of the surface based on the second calculation strategy.

Take a grid of the surface area as an example to illustrate the detailed calculation method. Suppose the projection range of the sample point cloud in the $xoy$ plane is ${(x, y) | x_{min} \leq x \leq x_{max}, y_{min} \leq y \leq y_{max}}$ . Generally, the point-cloud region can be moved to the first quadrant where the starting point $(0, 0)$ is a fixed point by means of coordinate transformation. The $xoy$ region can be divided into rectangles consisting of squares with the side length equal to $ε$ . Figure 1 shows the grid partitioning of the region. There are $M$ and $N$ rectangular meshes in the $x$ and $y$ directions. $M$ and $N$ can be calculated as in equation (3)

M = \frac{x_{max} - x_{min}}{ε}, N = \frac{y_{max} - y_{min}}{ε}

(3)

where $ε$ is an integer multiple of the point-cloud resolution $k_{s}$ , and the range of $ε$ is ${ε | ε_{min} \leq ε \leq ε_{\max}, k = 1, 2, 3 \dots}$ . $S (m, n)$ represents the m-th and n-th square in the direction of $x$ and $y$ . The central coordinate of $S (m, n)$ is $(x, y)$ , and the height is $z (x, y)$ .

Figure 1.

Division of the calculation region.

By fitting the minimum mean square plane $z (x, y)$ of the discrete point cloud in the $S (m, n)$ region, the residual mean square in the region is calculated as in equation (4). It is illustrated in two directions in a range of $0 - 0.01$ as shown in Figure 1

Δ H (m, n)^{2} = \frac{1}{n_{dot}} \sum_{i = x_{m min}}^{x_{m max}} \sum_{j = y_{n min}}^{y_{n max}} {[z (x_{i}, y_{j}) - z_{n} (x_{i}, y_{j})]}^{2}

(4)

where $Δ H (m, n)^{2}$ denotes the residual mean square of the $S (m, n)$ . $n_{dot}$ represents the number of points in $S (m, n)$ . $x_{m \min}$ , $x_{m max}$ , $y_{n min}$ , and $y_{n max}$ are the boundary coordinates of $S (m, n)$ , where $x_{m min} = (m - 1) ε$ , $x_{m max} = m ε$ , $y_{n min} = (n - 1) ε$ , and $y_{n max} = n ε$ . Equation (4) can be written as

Δ H (m, n)^{2} = {(\frac{k_{s}}{ε})}^{2} \sum_{i = (m - 1) ε}^{m ε} \sum_{j = (n - 1) ε}^{n ε} {[z (x_{i}, y_{j}) - z_{n} (x_{i}, y_{j})]}^{2}

(5)

$Δ H (m, n)$ , the RMS of the surface residuals of $S (m, n)$ , can be expressed as

\begin{matrix} Δ H (m, n) & = \sqrt{Δ H {(m, n)}^{2}} \\ = \sqrt{{(\frac{k_{s}}{ε})}^{2} \sum_{i = (m - 1) ε}^{m ε} \sum_{j = (n - 1) ε}^{n ε} {[z (x_{i}, y_{j}) - z_{n} (x_{i}, y_{j})]}^{2}} \end{matrix}

(6)

$H (ε)$ is created to denote the RMS of the whole surface $XoY$ , because it is related to the length of the edge. The incremental square roots of the surface RMS and coordinate variables show a power law relation.³⁰ The expression of $H (ε)$ is as in equation (7)

H (ε) ~ {(\sqrt{Δ x^{2} + Δ y^{2}})}^{3 - D}

(7)

Assuming $Δ x$ and $Δ y$ as $ε$ , we can get equation (8) by taking the logarithm of equation (7) as

\log (H (ε)) = (3 - D) \log (C_{1} + ε) + C_{2}

(8)

Under the representation of $ε - D$ coordinates, equation (9) can be derived by equation (8) as

D = 3 - \frac{\log H (ε) - C_{1}}{\log ε + C_{2}}

(9)

The value of $D$ is related to $(\log H (ε) / \log ε)$ . The constant terms $C_{1}$ and $C_{2}$ in the denominator represent the translation of the graph in a logarithmic graph, which has no impact on $D$ . Now the fractal dimension $D$ can be expressed as

D = lim_{ε \to 0} (3 - \frac{\log H (ε)}{\log ε})

(10)

This shows that the calculated value of $D$ is linearly related to $\log H (ε) / \log ε$ . Therefore, it can convert the calculation of $D$ to the fitting slope of $\log H (ε) / \log ε$ . The calculation steps of the 3R method are expressed as follows:

Step 1: Set the initial value of $ε$ to $ε_{0}$ .

Step 2: Divide the sample region into $M \times N$ rectangular grids according to equation (3).

Step 3: Calculate the $Δ H (m, n)$ of the region $S (m, n)$ according to equation (6) in turn.

Step 4: Calculate the $H (ε)$ of the whole sample surface.

Step 5: Change the value of $ε$ and return to Step 2 until $ε$ reaches $ε_{\max}$ .

Step 6: Go to Step 7 when $ε$ reaches $ε_{\max}$ .

Step 7: Fit the slope of $\log H (ε) - \log ε$ by the logarithmic values of calculated $ε - H (ε)$ data.

Step 8: Calculate the value of $D$ using equation (10).

Comparison of calculation results

In this article, the proposed 3R method is used to calculate the anisotropic and isotropic surfaces. To make a comparison, the DBC method, VM method, TPSA method, and the recently proposed 3D-RMS method are chosen to calculate the same surfaces. Then a comparison of these methods is carried out.

Application on isotropic surface

The isotropic surfaces with certain fractal dimensions are generated by equation (1). The fractal dimensions range from 2.1 to 2.9 with the step of 0.1. To simplify the comparison, the parameters given in Zuo et al. ²³ are used in calculations. The value range of $(x, y)$ is $(0, 1000]$ to make sure that the denominator is not 0, and $G = 2.39 \times 10^{- 7}$ , $γ = 1.5$ , $M_{0} = 10$ , $n_{max} = 22$ , $n_{1} = - 10$ .²³ The fractal surfaces with a dimension of 2.2, 2.4, 2.6, and 2.8 are shown in Figure 2.

Figure 2.

Isotropic fractal surface: (a) $D = 2.2$ , (b) $D = 2.4$ , (c) $D = 2.6$ , and (d) $D = 2.8$ .

For each given standard dimension $D$ , the results of the DBC, VM, TPSA, and 3D-RMS methods with the same parameters²³ are shown in rows 1–4 in Tables 1 –3, respectively. The absolute error and relative error of the 3R method are compared with those of the above methods as shown in Figure 3.

Table 1.

Calculation values of D for isotropic surface.

Theoretical D	2.1	2.2	2.3	2.4	2.5	2.6	2.7	2.8	2.9
DBC	2.1813	2.2511	2.3139	2.4002	2.4492	2.5302	2.5998	2.6706	2.7412
VM	2.1935	2.222	2.3064	2.3879	2.5185	2.5518	2.6531	2.6948	2.788
TPSA	2.1359	2.2438	2.3175	2.3548	2.4626	2.5799	2.6842	2.782	2.9057
3D-RMS	2.1653	2.2386	2.3231	2.4143	2.5096	2.6038	2.6989	2.7999	2.8908
3R method	2.0934	2.2096	2.2876	2.3884	2.5021	2.6042	2.6961	2.7992	2.8889

DBC: differential box counting; VM: variation method; TPSA: triangle prism area; RMS: root mean square.

Table 2.

Absolute errors for isotropic surface.

Theoretical D	2.1	2.2	2.3	2.4	2.5	2.6	2.7	2.8	2.9
DBC	0.0813	0.0511	0.0139	0.0002	0.0508	0.0698	0.1002	0.1294	0.1588
VM	0.0935	0.022	0.0064	0.0121	0.0185	0.0482	0.0469	0.1052	0.112
TPSA	0.0359	0.0438	0.0175	0.0452	0.0374	0.0201	0.0158	0.018	0.0057
3D-RMS	0.0653	0.0386	0.0231	0.0143	0.0096	0.0038	0.0011	0.0001	0.0092
3R method	0.0066	0.0096	0.0124	0.0116	0.0021	0.0042	0.0039	0.0008	0.0111

DBC: differential box counting; VM: variation method; TPSA: triangle prism area; RMS: root mean square.

Table 3.

Relative errors for isotropic surface.

Theoretical D	2.1	2.2	2.3	2.4	2.5	2.6	2.7	2.8	2.9
DBC	3.8714	2.3227	0.6043	0.0083	2.0320	2.6846	3.7111	4.6214	5.4759
VM	4.4524	1.0000	0.2783	0.5042	0.7400	1.8538	1.7370	3.7571	3.8621
TPSA	1.7095	1.9909	0.7609	1.8833	1.4960	0.7731	0.5852	0.6429	0.1966
3D-RMS	3.1095	1.7545	1.0043	0.5958	0.3840	0.1462	0.0407	0.0036	0.3172
3R method	0.3143	0.4364	0.5391	0.4833	0.0840	0.1615	0.1444	0.0286	0.3828

DBC: differential box counting; VM: variation method; TPSA: triangle prism area; RMS: root mean square.

Figure 3.

Comparative diagram of absolute errors and relative errors for the isotropic surface.

Application on anisotropic surfaces

The surface parameters of anisotropic surfaces are different in different cross-sectional directions. Therefore, it is not wise to measure the whole surface with a single surface curve in a certain direction. When it comes to the anisotropy surface, the second strategy is the only method to use.

An anisotropic surface with a certain fractal dimension can be obtained by generating a curve in the directions of $x$ or $y$ and stretching along the other direction. In this article, the curve is generated in the $x$ direction and then stretched along the $y$ direction. It is necessary to note that this approach is fundamentally different from the first strategy, which is mentioned in section “Fractal dimension calculation method based on the rms of regional residuals.” This kind of surface has a fractal dimension $D_{x}$ in the $x$ direction. The fractal dimension $D$ of the whole surface equals $1 + D_{x}$ , but this is just a special case.

Equation (2) denotes the expression of the 2-DW-M fractal function. The fractal dimensions range from 2.1 to 2.9 with the step of 0.1. The value range of $(x, y)$ is $(0, 1000]$ , and $G = 2.39 \times 10^{- 7}$ , $γ = 1.5$ , $M_{0} = 10$ , $n_{\max} = 22$ , $n_{1} = - 10$ . The surfaces with dimensions of 2.2, 2.4, 2.6, and 2.8 are shown in Figure 4.

Figure 4.

Anisotropic fractal surface: (a) $D = 2.2$ , (b) $D = 2.4$ , (c) $D = 2.6$ , and (d) $D = 2.8$ .

For each given standard dimension $D$ , the results of the DBC, VM, TPSA, and 3D-RMS methods with the same parameters are shown in rows 1–4 in Tables 4 –6²³ respectively. The absolute error and the relative error of the 3R method are compared with those of the above methods as shown in Figure 5.

Table 4.

Calculation values of D for anisotropy surface.

Theoretical D	2.1	2.2	2.3	2.4	2.5	2.6	2.7	2.8	2.9
DBC	2.2652	2.3095	2.3503	2.4027	2.454	2.5869	2.6518	2.7329	2.7775
VM	2.2461	2.2837	2.3251	2.4117	2.4767	2.5727	2.6717	2.7223	2.7646
TPSA	2.2238	2.2851	2.352	2.4267	2.5766	2.6435	2.7244	2.8323	2.8546
3D-RMS	2.1881	2.2423	2.3039	2.3973	2.4988	2.5973	2.6946	2.7976	2.8945
3R method	2.1305	2.2206	2.3123	2.4045	2.4951	2.6023	2.7034	2.7951	2.8909

DBC: differential box counting; VM: variation method; TPSA: triangle prism area; RMS: root mean square.

Table 5.

Absolute errors for anisotropy surface.

Theoretical D	2.1	2.2	2.3	2.4	2.5	2.6	2.7	2.8	2.9
DBC	0.1652	0.1095	0.0503	0.0027	0.046	0.0131	0.0482	0.0671	0.1225
VM	0.1461	0.0837	0.0251	0.0117	0.0233	0.0273	0.0283	0.0777	0.1354
TPSA	0.1238	0.0851	0.052	0.0267	0.0766	0.0435	0.0244	0.0323	0.0454
3D-RMS	0.0881	0.0423	0.0039	0.0027	0.0012	0.0027	0.0054	0.0024	0.0055
3R method	0.0305	0.0206	0.0123	0.0045	0.0048	0.0023	0.0034	0.0048	0.0090

DBC: differential box counting; VM: variation method; TPSA: triangle prism area; RMS: root mean square.

Table 6.

Relative errors for anisotropy surface.

Theoretical D	2.1	2.2	2.3	2.4	2.5	2.6	2.7	2.8	2.9
DBC	7.8667	4.9773	2.1870	0.1125	1.8400	0.5038	1.7852	2.3964	4.2241
VM	6.9571	3.8045	1.0913	0.4875	0.9320	1.0500	1.0481	2.7750	4.6690
TPSA	5.8952	3.8682	2.2609	1.1125	3.0640	1.6731	0.9037	1.1536	1.5655
3D-RMS	4.1952	1.9227	0.1696	0.1125	0.0480	0.1038	0.2000	0.0857	0.1897
3R method	1.4524	0.9364	0.5348	0.1875	0.1920	0.0885	0.1259	0.1714	0.3103

DBC: differential box counting; VM: variation method; TPSA: triangle prism area; RMS: root mean square.

Figure 5.

Comparative diagram of absolute errors and relative errors for the anisotropic surface.

Analysis of results

For the isotropic and anisotropic surfaces, the results obtained by the 3R method proposed in this article, and the DBC, VM, TPSA, and 3D-RMS methods have been compared, respectively, in sections “Application on isotropic surface” and “Application on anisotropic surfaces,” and are shown in Tables 1 –6. From Figures 3 and 5, there is no doubting that the 3R method has the smallest calculation error among these methods. The calculation accuracy of the DBC method depends on the box size. At a small box size condition, the fitting error is very large, and if the size is too large, the calculation results tend to be meaningless. For the VM method, the calculation formula is complex and time-consuming and the accuracy is no better than the DBC method. These two methods have large relative errors at both very low and very high dimensions. When calculating the isotropic and anisotropic surfaces, the maximum relative errors of the DBC and VM methods are 5.4%, 7.8% and 4.5%, 6.9%, respectively. The TPSA method uses special points to represent the entire surface, which leads to the reduction in precision. There are no obvious trends of error in Figures 3 and 5, because of the insufficient use of data. Their relative maximum errors are 1.9% and 5.8% in the isotropic and anisotropic surfaces. For the RMS method, it has a better performance than the DBC, VM, and TPSA methods. However, excessive pursuit of linearity leads to a weak performance in low fractal dimension. The relative maximum errors are 3.1% and 4.1% in the isotropic and anisotropic surfaces. For isotropic surfaces, the maximum relative error of the 3R method is only 0.5%. And for anisotropic surfaces, the relative errors of the 3R method are less than 0.5% in most cases, except in two computational cases that are near 1%, which is far less than other algorithms. Compared with those methods, only 3D-RMS can achieve similar results. However, when the fractal dimension is 2.1 and 2.2, the 3R method is more accurate than the 3D-RMS method with margins of 2.7% and 1%. The results show that the 3R method has the highest accuracy and the best stability with comprehensive consideration of the outcomes in both the isotropic and anisotropic surfaces with a large applied range among the methods, which demonstrates that the proposed method can be applied in the calculation of fractal dimension of both the isotropic and anisotropic surfaces.

Surface modeling method based on the 3R method

The difficulty of surface modeling machined parts lies in the reproduction of micro-geometric error information. The surface can be regarded as the superposition of a roughness, waviness, and form error contour whose wavelength range is greater than $λ_{s}$ shown in Figure 6. These parameters intuitively reflect the mechanical properties of the surface, thus ensuring that the constructed model has the same parameters as the actual parts and is the basis for further research on the performance of virtual assembly.

Figure 6.

Surface profile.

This is the key to constructing the surface model using the 3R method to calculate the fractal dimension of the actual parts surface. But the value of $G$ has not been determined. To reproduce the surface parameters of the model, it adopts the $G$ that is related to $A$ and equals 1 in equation (1). The surface contour components are separated by wavelet analysis, and each component is reconstructed and integrated according to the actual parameters. Using this method, the surface parameters of the model are consistent with the actual parameters, and the surface information hidden by $A$ that equals 1 is released. Finally, the virtual integration between the virtual model and the actual parts is realized. Wavelet analysis is used to extract the above surface components from the surface profile. The surface morphology $z (x, y)$ is used as the input. The wavelet basis function is selected to decompose $z (x, y)$ . The signal is filtered and the low-frequency and high-frequency information are separated twice. After the first wavelet decomposition, the original signal is separated into low-frequency information, horizontal high-frequency information, vertical high-frequency information, and diagonal high-frequency information, among which, meaningless high-frequency components must be discarded. Low-frequency information obtained after $N$ times decomposition is defined as $z (x, y)_{N}$ . The formulas for calculating the $N_{i}$ values of each contour parameter are as follows¹²

N_{i} = [\frac{\ln λ_{i} - \ln λ_{s}}{\ln 2}] + 1, i \in {f, c, s}

(11)

Wavelet reconstruction is an inverse process of decomposition. After wavelet transform, the roughness, waviness, and form error profile are obtained. The correction coefficients $k_{R_{a}}$ , $k_{W_{z}}$ , and $k_{F_{p}}$ ¹² are introduced to integrate the components of each surface contour. Then information about the independent scale parameter $G$ is released. The final model is the superposition of roughness, waviness, and form error profile after the integration of wavelet analysis and surface morphology according to equation (12) as

z = z_{f} + z_{c} + z_{s}, {\begin{matrix} z_{f} = k_{F_{p}} \cdot z_{N_{f}} \\ z_{c} = k_{W_{z}} \cdot z_{N_{c}} \\ z_{s} = k_{R_{a}} \cdot z_{N_{s}} \end{matrix}

(12)

Case study

In this article, the VTM-200/F5 turning and milling composite machining center made by Qinchuan Machine Tool & Tool (Group) Corp. is taken as a research object as shown in Figure 7(a), taking the slide of the $x - axis$ feed component as an example. The fractal dimension of the surface of the slide is inversely calculated by the 3R method based on the point-cloud data obtained from the surface of the part. The calculated value of $D$ is introduced into equation (1); then the surface morphology model is established. The surface parameters are extracted through the wavelet transform, and finally, the microtopography model is achieved.

Figure 7.

Model of the case: (a) Physical prototype of the VTM200/F5 and the slide, and (b) Schematic diagram of linear guideway parameters.

Some parameters of the slide are as follows: $M = 58$ , $W_{1} = 63$ , $F = 75$ , and $d_{2} = 18$ as shown in Figure 7(b). The sample of the point-cloud data is taken from the area of the slide with the length of a side equal to 25 mm, and the sampling interval 0.05 mm.

The initial value of $ε_{0}$ is 0.1. The region of the point cloud is zoned and decomposed into a square array with a side length of 0.1. Minimum mean square fitting is carried out for each region in turn, and the residual error of the point cloud is obtained according to the 3R method. The value of $H (ε_{0})$ is calculated and recorded with $ε_{0}$ .

The value of $ε$ is increased by 0.1 and the corresponding $H (ε)$ is calculated according to equation (6). Then each set of data $ε$ and $H (ε)$ is recorded until $ε$ reaches the maximum. Each $[ε, H (ε)]$ point is drawn in a logarithmic graph as shown in Figure 8(a). The slope of fitting is calculated to be 0.52. According to equation (11), the calculated value of the fractal dimension of the surface is 2.48. The obtained sampling point-cloud is shown in Figure 8(b).

Figure 8.

(a) $\log ε - \log H (ε)$ plot, and (b) Sampling point cloud of the case.

The surface of the slide is reconstructed using the W-M function with $D = 2.48$ . A is assumed to equal 1 as shown in Figure 9(a). To release the information loss, it is necessary to evaluate the surface structure and obtain the parameters of the surface model. Wavelet analysis of $z (x, y)$ is performed 1 time, 4 times, and 8 times, respectively, according to equation (11). The form error, waviness, and roughness profile are separated as Figure 9(b)–(d).

Figure 9.

Wavelet decomposition: (a) W-M fractal surface with $D = 2.48$ , $A$ = 1, (b) Form error, (c) Waviness, and (d) Roughness.

The surface correction coefficients are calculated according to the design parameters as shown in Table 7. Then the hidden surface height information is released with a scaling factor $A$ of 1, and the actual surface of the slide wear is synthesized as shown in Figure 10.

Table 7.

Designed value, calculated value, actual parameter, and coefficient of correction.

	Roughness (Ra)	Waviness (Wz)	Form error (Fp)
Designed value	0.8	0.0064	15 μm/300 mm
Calculated value	1.62E + 05	17.3755	32.5578
Actual parameter	0.79	0.0062	15 μm/300 mm
Coefficient of correction	4.88E-06	3.57E-04	1.54 E-06

Figure 10.

Reconstruction of surface: (a) Contour surface, (b) Form error, (c) Waviness, and (d) Roughness.

The reconstructed surface is imported into the computer-aided design (CAD) system to obtain the point-cloud model, the grid model, and the surface model in virtual reality environment, as shown in Figures 11 and 12.

Figure 11.

Reconstructed model: (a) Point-cloud model, and (b) Gridding model.

Figure 12.

Virtual assembly of guide rail in VTM-200/F5 turn-milling composite center: (a) Surface model, (b) Guiderail model, and (c) Assembly model of machine.

Finally, the modeling result was compared with the other two methods from other related literatures, which could be obtained from Zhang et al.³ and Wang et al.⁵. The modeling results are shown in Figure 13, and the details can be seen in Table 8. The traditional fractal modeling method can build the computer-aided geometric design (CAGD) model based on primary W-M theory, which is simple with less storage data, but has a bad efficiency and an unsatisfied result. The method can only be a simple representation of the surface. A novel modeling method can produce point-cloud model and surface model based on nonuniform rational basis spline (NURBS) surface. However, the good result depends on complex operation and a large amount of data. The method is cost-effective to apply to the modeling of complex and special surfaces and the following research. The surface modeling method based on the 3R method proposed in this article can produce the point-cloud model and surface model based on W-M theory mixed with reconstruction of model by wavelet transform. Compared with the three methods, it is simple and logic and does not require too much data as well. Moreover, it takes measures for maintaining surface parameters by wavelet decomposition and reconstruction, which is the most obvious advantage over others.

Figure 13.

Comparison of modeling results: (a) Fractal modeling method, (b) A novel modeling method, and (c) A surface modeling method based on 3R method proposed in this article.

Table 8.

Comparison of modeling results and modeling methods.

Modeling Methods	Fractal modeling method⁵	A novel modeling method³	A surface modeling method based on 3R method
Theory	W-M theory	NURBS surface	W-M theory and reconstruction of model by wavelet transform
Formats	CAGD model	Point-cloud, surface model	Point-cloud, surface model
Measures for maintaining surface parameters?	No	No	Yes, wavelet decomposition and reconstruction.
Complexity	Simple	Complex	Simple
Efficiency	Bad	Good	Good
Data size	Small	Large	Medium

W-H: Weierstrass-Mandelbrot; NURBS: nonuniform rational basis spline; CAGD: computer-aided geometric design.

The surface model constructed by the 3R method proposed in this article is helpful in maintaining the surface morphology of parts. From Figure 8(a) it can be seen that the linearity of the slope fitting is good, which verified the feasibility of the 3R method. In the constructed virtual model, the surface roughness information of the actual parts were maintained, and the virtual model was realized. It is proved that the 3R method can be used in a situation such as virtual reality, virtual prototyping, or digital twin application.

Conclusion

The following conclusions are drawn:

A 3R method was proposed in this article to solve the problems involved in 3-D fractal dimension calculation. This method can take full advantage of the surface point-cloud data and obtain calculations that are closest to the real value. Moreover, it maintained good stability in calculation accuracy. By comparing the results of the isotropic and anisotropic surfaces with those of other traditional methods, the relative error of the proposed method was controlled within 0.5.

According to the 3R method, the fractal dimension of the real part surface was calculated, and the digital model of the part for virtual assembly of the product was constructed. Then, the roughness, waviness, and flatness components were extracted by wavelet transform, and the surface was reconstructed according to the design parameters and the hidden surface information related to $G$ was released. The contour features of the actual parts were maintained.

The 3R method was validated in the application of the virtual assembly of the guiderail of the VTM-200/F5 turn-milling composite center. The established virtual assembly surface model can be further applied to predict the virtual assembly accuracy, which will be studied in future research.

Prospect

The assembly precision of mechanical parts is an important index to measure the product performance. The factors that determine the assembly quality of the product can be divided into manufacturing factors and assembly factors. Reliable prediction of assembly performance is of guiding significance to assembly activities. The contact surfaces in mating zone can be represented by the digital model based on the proposed method shown in Figure 14. The manufacturing factor refers to the dimension deviation in the geometric plane of the part. The base surface of the part can be achieved by fitting the virtual surface model, and the irregular surface of the fractal surface can be viewed as the manufacturing error. We are trying to propose a potential tolerance transfer theory to predict the assembly precision based on the modeling method in this article and hypothesis above. And the functional requirement (FR) will be the research object based on the virtual assembly contact model. As shown in Figure 14, the geometric tolerance of A1 relative to the datum after assembly will be an example of FR, which will be a case study in the future research.

Figure 14.

Potential experiment in the following research.

Footnotes

Declaration of conflicting interests

The author(s) declared no potential conflicts of interest with respect to the research, authorship, and/or publication of this article.

Funding

The author(s) disclosed receipt of the following financial support for the research, authorship, and/or publication of this article: The National Natural Science Foundation of China (51875516), the Youth Funds of the State Key Laboratory of Fluid Power and Mechatronic Systems of Zhejiang University (SKLoFP _ QN _ 1702), Collaborative Innovation Center of High-end Manufacturing Equipment, and the Natural Science Foundation of Zhejiang Province (LY18E050001).

ORCID iDs

Heng Li

Lemiao Qiu

References

Wang

, et al. Live parametric design modifications in CAD-linked virtual environment. Int J Adv Manuf Tech 2010; 50(9–12): 859–869.

Zhu

Peng

, et al. An improved horizontally reversible plow design based on virtual assembly semantics and constraint. J Mech Sci Technol 2016; 30(1): 257–266.

Zhang

Jin

, et al. A novel modelling method of geometric errors for precision assembly. Int J Adv Manuf Tech 2018; 94(1–4): 1139–1160.

Qiu

Liu

, et al. Hybrid dimension based modeling of part surface topography and identification of its characteristic parameters. Appl Surf Sci 2012; 258(18): 7082–7093.

Wang

Chen

, et al. Synthesis of fractal geometry and cagd models for multi-scale topography modelling of functional surfaces. J Cent South Univ T 2011; 18(5): 1493–1501.

Wang

Yang

Yuan

XG.

Evaluation of the wavelet transform method for machined surface topography 2: fractal characteristic analysis. Tribol Int 2003; 36(7): 527–535.

Zhou

Zhu

, et al. The three-point sinuosity method for calculation the fractal dimension of machined surface profile. Fractals 2015; 23(02): 1550016.

Rahimi

Bagheri

Masihi

. Characterization and estimation of reservoir properties in a carbonate reservoir in southern iran by fractal methods. J Pet Explor Prod Technol 2018; 8(1): 31–41.

Wang

. Fractal function estimation via wavelet shrinkage. J R Stat Soc 1997; 59(3): 603–613.

10.

Josso

Burton

Lalor

. Frequency normalised wavelet transform for surface roughness analysis and characterisation. Wear 2002; 252(5): 491–500.

11.

Ausloos

Berman

. A multivariate weierstrass-mandelbrot function. Proc R Soc Lond Ser A 1985; 400(1819): 331–350.

12.

Qiu

Liu

Zhou

, et al. Modeling of part surface topography based on revised multi-scale altitude field. J Comput-Aid Des Comput Graph 2012; 24(12): 1631–1639.

13.

Liao

Zhang

Feng

, et al. Identification of contact stiffness of shrink-fit tool-holder joint based on fractal theory. Int J Adv Manuf Tech 2017; 90(5–8): 2173–2184.

14.

Zhao

, et al. A geometrical-mechanical-thermal predictive model for thermal contact conductance in vacuum environment. Proc IMechE, Part B: J Engineering Manufacture 2015; 230(8): 1451–1464.

15.

Sarkar

Chaudhuri

. An efficient differential box-counting approach to compute fractal dimension of image. IEEE T Syst Man Cyb 1994; 24(1): 115–120.

16.

Thomas

Sankar

. Fractal features based on differential box counting method for the categorization of digital mammograms. Inform Syst 2010; 2: 11–19.

17.

Cantoni

. Recent issues in pattern analysis and recognition. Berlin: Springer, 1989.

18.

Santis

Fedi

Quarta

. A revisitation of the triangular prism surface area method for estimating the fractal dimension of fractal surfaces. Ann Geophys 1997; 40(4): 811–821.

19.

Dubuc

Zucker

Tricot

, et al. Evaluating the fractal dimension of surfaces. P Roy Soc A-Math Phy 1989; 39(3): 1500–1513.

20.

Dhu

Dentith

Hillis

. Enhancement of airborne magnetic data using the variation method of fractal dimension estimation. Explor Geophys 2000; 31(2): 58–65.

21.

Lin

Wang

Chen

, et al. Two-stage method for fractal dimension calculation of the mechanical equipment rough surface profile based on fractal theory. Chaos Solitons Fract 2017; 104(4): 495–502.

22.

Zuo

Zhu

Zhou

, et al. Estimation of fractal dimension and surface roughness based on material characteristics and cutting conditions in the end milling of carbon steels. Proc IMechE, Part B: J Engineering Manufacture 2015; 231(8): 1423–1437.

23.

Zuo

Zhu

Zhou

, et al. A new method for calculating the fractal dimension of surface topography. Fractals 2015; 23(03): 1550022.

24.

Jing

Feng

Wei

, et al. Investigation on the surface morphology of

s i_{3} n_{4}

ceramics by a new fractal dimension calculation method. Appl Surf Sci 2016; 387: 812–821.

25.

Moktadir

Sato

. Wavelet characterization of the submicron surface roughness of anisotropically etched silicon. Surf Sci 2000; 470(1): L57–L62.

26.

Wang

Shi

Liao

, et al. Using wavelet packet transform for surface roughness evaluation and texture extraction. Sensors 2017; 17(4): 933.

27.

Tangjitsitcharoen

Thesniyom

Ratanakuakangwan

. A wavelet approach to predict surface roughness in ball-end milling. Proc IMechE, Part B: J Engineering Manufacture 2015; 231(14): 2468–2478.

28.

Pang

Kuang

, et al. Study on the extraction and reconstruction of arbitrary frequency topography from precision machined surfaces. Proc IMechE, Part B: J Engineering Manufacture 2019; 233: 1772–1780.

29.

Majumdar

Tien

. Fractal characterization and simulation of rough surfaces. Wear 1990; 136(2): 313–327.

30.

Falconer

. Fractal geometry: mathematical foundations and applications. New York: Wiley, 1990.

A surface modeling method for product virtual assembly based on the root mean square of the regional residuals

Abstract

Keywords

Introduction

Overview of approach

Calculation of fractal dimension by the area residuals method

Surface modeling based on fractal theory

Fractal dimension calculation method based on the RMS of regional residuals

Comparison of calculation results

Application on isotropic surface

Application on anisotropic surfaces

Analysis of results

Surface modeling method based on the 3R method

Case study

Conclusion

Prospect

Footnotes

Declaration of conflicting interests

Funding

ORCID iDs

References