1 Introduction

Abrasive waterjet (AWJ) is a non-traditional green machining method being widely used in the world today. AWJ is formed by adding abrasive particles into the high-speed water beam, and the material removal is mainly achieved by the shearing effect of abrasive particles [1]. This technology is able to machine a wide range of materials because of its unique advantages like higher versatility, no heat affected zone, lower cutting forces, and good environmental performance [2]. During its working process, nearly no dust or harmful particles are produced, which is friendly to the environment [3]. The performance of AWJ processing is affected by various parameters, among which the waterjet pressure, the abrasive flow rate, the traverse speed, and the standoff distance are the main ones [4].

In order to improve the cutting ability of AWJ, many researchers are focusing on investigating the effects of machining parameters on the roughness (Ra) and taper (Kt) of the cut surface and kerf. For example, Arvind et al. [5] experimentally studied the influence of AWJ processing parameters on the cutting quality of Inconel 718 with the use of response surface methodology (RSM). They found that both the abrasive flow rate and traverse speed are the most substantial parameters. Similar results were also obtain by Joel et al. [6], who used the Taguchi method linked with the gray relation analysis to investigate the machinability of AA7075 aluminum alloy by AWJ. Moreover, Ahmed et al. [7] used experimental design and statistical modeling techniques to make an investigation on the influence of AWJ cutting parameters on the surface roughness. As a result, the waterjet pressure and traverse speed were claimed as significant parameters. Yuvaraj et al. [8] studied the cutting performance of cryogenic-assisted AWJ under different waterjet pressures, abrasive sizes, and AWJ impact angles. Xiong et al. [9] put forward a new cutting strategy that reverses cutting with variable standoff distance to improve the cutting performance of Ti6Al4V. Besides, Yang et al. [10] studied the effects of processing parameters on the cutting capacity and quality with the monolithic abrasive material and corresponding mixing abrasive materials, respectively. They found that the variation of abrasive flow rate greatly determines the cutting performance. These investigations indicate that by optimizing the machining parameters of AWJ, the cutting quality of materials can be significantly improved.

On the other hand, numerous studies in the literature have already shown that waterjet pressure is one of the most significant factors affecting the cutting ability of AWJ and the cutting quality [11,12,13]. It can be claimed that a higher waterjet pressure generally results in better cutting qualities, especially for hard materials [14, 15]. Our previous cutting experiments also showed that the waterjet pressure should be as high as 400 MPa when cutting U71Mn material if satisfied surface quality needs to be obtained [16]. Therefore, experiments and investigations are mainly performed at ultra-high pressures. Almost all, the studies on AWJ cutting are conducted at pressures above 300 MPa, and so far, few investigations on AWJ cutting at pressures below 200 MPa can be found in the literature. But it is known that a higher pump pressure means that the manufacturing and maintenance cost will be largely raised and the service life will be greatly reduced at the same time [17]. Up to now, whether a relatively low pressure waterjet can cut materials with a high quality as that achieved by ultra-high pressure waterjets remains unclear.

In the present study, an attempt was made to discover the cutting ability of AWJ with a relatively low pressure. By varying the traverse speed, standoff distance, abrasive flow rate, and the number of cutting pass, the cutting quality of 5052 aluminum alloy under the impact of AWJ at 150 MPa was studied. The cutting quality was then compared with an ultra-high pressure of 350 MPa. This study could help obtain a high cutting quality of AWJ at a low waterjet pressure by using reasonable machining parameters.

2 Experimental procedure and facilities

2.1 Specimen

As aluminum alloy 5052 has superior manufacturability such as formability, corrosion resistance, and weldability, it is being widely employed in aircraft fuel tanks, autonomous body structures, and sheet metal parts of marines [18]. Thus, aluminum alloy 5052 was used as the cutting specimen in this study, and the chemical composition and main mechanical properties are displayed in Tables 1 and 2, respectively [19, 20]. The dimensions of length, width, and thickness of the specimen were 20 mm, 10 mm, and 5 mm, respectively.

Table 1 Chemical composition of aluminum alloy 5052
Table 2 Main mechanical properties of aluminum alloy 5052

2.2 Equipment

All the cutting tests were performed using an AWJ platform (Model: APW2016BA-18) shown in Fig. 1. The platform was equipped with a five-axis cutting head and a pump with the maximum ultra-high pressure up to 420 MPa. The AWJ device also had an abrasive delivery system that can adjust the abrasive flow rate ranging from 70 to 880 g/min.

Fig. 1
figure 1

AWJ devices

The roughness of the cut surface, Ra, was obtained by the contact-type surface measuring instrument (Mitutoyo SJ-210). Three different locations on the surface of each specimen were selected for measurement, and the average values were used to minimize the errors. The measurement length was 6 mm, and the movement speed of the probe was 0.5 mm/s. The calculation results and surface roughness waveform can be displayed on the device. The instrument and measurement method are shown in Fig. 2.

Fig. 2
figure 2

Mitutoyo SJ-210 and measurement method

The taper of the cut kerf, Kt, was also used for evaluating the quality of the cut surface, and it was obtained by a three-dimensional profiler (Model: NanoFocus μscan) illustrated in Fig. 3. The profiler was used to collect the contour shape of the cut surface and measure the width of the upper and lower cuts. Then, Kt could be obtained using the following equation [21]

$$K_{{\text{t}}} = \tan^{ - 1} \left( {\frac{{W_{{\text{t}}} - W_{{\text{b}}} }}{2h}} \right)$$
(1)

where Wt, Wb, and h are, respectively, denoted as the width of the upper kerf, the width of the lower kerf, and the thickness of the specimen.

Fig. 3
figure 3

NanoFocus μscan profiler

2.3 Experimental design

During all the cutting tests, the waterjet impact angle, the garnet abrasive size, and the focusing nozzle diameter were kept as 90°, 80 mesh, and 1.02 mm, respectively. Preliminary cutting experiments had been performed, and results showed that 150 MPa was the minimum pressure for cutting through the aluminum alloy 5052 specimen at a single cutting. In the meantime, a relatively high cutting quality of Ra = 4.842 μm and Kt = 1.118° could be obtained at a much higher pressure of 350 MPa with the traverse speed of 100 mm/min, standoff distance of 2 mm, and abrasive flow rate of 390 g/min. Thus, 150 MPa was used as the relatively low pressure, and 350 MPa was used as the ultra-high pressure for comparison.

In this study, two cutting methods were used to improve the machining quality at the relatively low pressure of 150 MPa. One was optimizing the main process parameters, which were the traverse speed, the standoff distance, and the abrasive flow rate, the other was using double-pass cutting with alternate directions.

RSM, which is a statistical method for solving multivariate problems, was used in company with the Central Composite Design (CCD) model. One advantage of CCD over Box-Behnken Design (BBD) and other design techniques of the experiment is its design flexibility, which allows for increased factor levels by adding axial points [22]. In general, the basic form of the multivariate quadratic response surface regression model is shown as follows [23].

$$Y = b_{0} + \sum\limits_{i = 1}^{\infty } {b_{i} X_{i} + } \sum\limits_{i = 1}^{\infty } {b_{ii} X_{i}^{2} + } \sum\limits_{i = 1}^{\infty } {\sum\limits_{j > 1}^{\infty } {b_{ij} X_{i} X_{j} + } \varepsilon }$$
(2)

where Y is the response factor (Ra, Kt), b0 is the regression intercept, bi, bii, and bij are regression coefficients, ε is the random experimental error, and Xi, Xj are independent variables of dimensionless coded.

A model of three factors at five levels was adopted to obtain the optimum cutting parameters. Coding factors A, B, and C stand for the traverse speed, the standoff distance, and the abrasive flow rate, separately. For each factor, the values of levels 2 and 4 were determined by the preliminary experiment, and the other three levels were acquired by the CCD model. All the process parameters are summarized in Table 3.

Table 3 Levels of the cutting parameters in the experiment

3 Results and discussion

A total of 40 cutting tests were performed at the relatively low pressure of 150 MPa. In more specific terms, 20 tests were under single-pass cutting, and the other 20 were under double-pass cutting. The values of Ra and Kt of each test are displayed in Table 4, as well as those obtained at the ultra-high pressure of 350 MPa in the preliminary experiment, for the convenience of comparison.

Table 4 Ra and Kt values at different cutting conditions

3.1 Cutting quality improvement by optimizing process parameters

The optimization of the three process parameters was studied under the condition of single-pass cutting. RSM was used for clarifying the influence of process parameters on the response metrics. It also helped to establish the quadratic regression equation models of Ra and Kt considering the above cutting parameters. The final quadratic regression equation models of Ra and Kt according to the coding factors are given in Eqs. 3 and 4, respectively.

$$R_{{\text{a}}} = 12.59 + 2.32A - 0.7419B - 1.94C - 1.27AC - 1.63A^{2} + 0.5473C^{2}$$
(3)
$$K_{{\text{t}}} = 1.13 + 0.3164A + 0.1273B + 0.0955C + 0.0743C^{2}$$
(4)

However, it should be pointed out that in double-pass cutting, due to the polishing and trimming effects of the secondary cutting, the influence of various factors on cutting quality is weakened, and the prediction model of quadratic regression equation is not reliable. Therefore, only the surface quality prediction model of single-pass cutting is analyzed in this paper.

Analysis of variance (ANOVA), generally used for significance testing, was applied to evaluate the significance of the cutting parameters. The ANOVA analysis result of Ra under 150 MPa single-pass cutting is shown in Table 5. The F-value of the model is 52.71, and the P value is less than 0.05, which indicates that the established model is significant. Each item with p value less than 0.05 has a significant influence on the model as a whole. As can be seen from Table 5, A, B, C, AC, A2, C2 are the significant model terms. Similarly, the ANOVA result for the Kt of 150 MPa single-pass cutting is shown in Table 6, from which it can be found that the Kt is influenced significantly by the model terms of A, B, C, and C2.

Table 5 ANOVA for Ra
Table 6 ANOVA for Kt

The normal plots of residuals of Ra and Kt are shown in Fig. 4. All residuals are approximately evenly distributed along a straight line, indicating that the error of the regression model obtained is small and the accuracy is high. Therefore, it can be used as a basis for predicting the results of response variables [24].

Fig. 4
figure 4

Residual plots of response a Surface roughness, b Kerf taper

The approximate degree of the actual values and predicted values of Ra and Kt are shown in Fig. 5. The actual values and predicted values are generally distributed near the central line, which has a good linear fitting relationship [25]. This shows the good applicability of the model, which also confirms that the established model has high precision in predicting Ra and Kt.

Fig. 5
figure 5

Predicted versus Actual a Surface roughness, b Kerf taper

Figure 6a-c display the response surface results of Ra. In Fig. 6a, the effect of the interaction between the standoff distance and traverse speed on Ra is shown under the abrasive flow rate of 390 g/min. For lower transverse speeds and higher standoff distances, the Ra will decrease. This is due to the reason that the cutting time of AWJ is increased [26]. The interaction between abrasive flow rate and traverse speed on Ra is shown in Fig. 6b, where the standoff distance remains unchanged at 1.5 mm. For a combination of a high abrasive flow rate and a low traverse speed, a decrease in Ra is observed. This is because the increase in abrasive flow rate increases the number of grits per unit time, which increases the cutting area of grits. As a consequence, the waterjet capacity is improved, making the processed surface cleaner [27]. Figure 6c is the 3D response surface of abrasive flow rate and standoff distance at a constant traverse speed of 75 mm/min. It can be seen that a smaller Ra can be obtained at an abrasive flow rate of 710 g/min and a standoff distance of 2.34 mm. This is because the increase in the standoff distance enlarges the acceleration time of AWJ and increases the grit kinetic energy, which in turn enhances the processing ability of AWJ.

Fig. 6
figure 6

3D response surface of surface roughness

Figure 7a-c portrays the 3D surface plot of the Kt with traverse speed, standoff distance, and abrasive flow rate. As can be seen from Fig. 7a, with the decrease in traverse speed and standoff distance, the Kt shows a decreasing trend. The minimum Kt can be obtained at the standoff distance of 0.66 mm and traverse speed of 33 mm/min. This is because the reduction in traverse speed increases the material removal time, resulting in similar kerf widths at the exit and entrance of the kerf. The reduction in the target distance leads to the reduction in the diffusion angle of the AWJ, and the waterjet beam is concentrated in a smaller angular range [28]. Figure 7b and c shows that there is an intermediate abrasive flow rate of about 350 g/min that makes the Kt minimum. As the abrasive flow rate decreases, the contact between the grits also decreases. Thus, the kerf entrance and the kerf taper are decreased. However, an extremely low abrasive flow rate can lead to a sharp reduction in the AWJ’s cutting capability and the kerf width at the exit is small, resulting in a larger taper [29].

Fig. 7
figure 7

3D response surface of kerf taper

RSM is also an optimization method where the goal of optimization is to determine the optimal combination of parameters to obtain the optimal output response. The parameter optimization can achieve different optimization objectives, such as achieving the maximum or minimum value of the output response or achieving a specific target value. For multi-objective optimization, each optimization objective has a certain importance. The least important optimization goal is represented by ( +), and the most important optimization goal is represented by (+ +  +  + +). Table 7 shows the relevant parameter optimization settings. In this study, the optimization process has two main objectives. Determine the minimum Ra and the minimum Kt for the cutting process using the maximum importance coefficient (+ +  +  + +), other parameters are normalized to find the combination of parameters that satisfies the objective proposal.

Table 7 Parameter optimization settings

The optimization results obtained based on the parameter optimization setting are Ra = 4.55 μm and Kt = 0.149°, with a corresponding expected value of 84.6% as shown in Table 8. At this time, the traverse speed is 33 mm/min, the standoff distance is 0.66 mm, and the abrasive flow rate is 339 g/min. Compared with the experimental results of the control group, Ra is reduced by 6.03%, and Kt is reduced by 86.67%.

Table 8 Optimization results in Ra and Kt

3.2 Cutting quality improvement by the double-pass cutting strategy

In addition to the 20 specimens obtained at 150 MPa by single-pass cutting, another set of 20 specimens was also cut by 150 MPa double-pass cutting with alternate directions using the same cutting parameters. Then, using the optimal parameters obtained above, the specimens were cut by the two cutting strategies under the low-pressure waterjet condition, and the specimens of the high-pressure control group are shown in Fig. 8. It can be found that under 150 MPa single-pass cutting conditions, the presence of oblique stripes at the bottom of the cut surface can be seen in Fig. 8a. While under 350 MPa single-pass cutting, the trace of the stripe fades significantly and becomes a straight stripe. The reason is that the increase in pressure enhances its cutting ability and effective material removal can be achieved at the bottom of the specimen as well. With 150 MPa double-pass cutting, the stripes are almost invisible on the cut surface, and the cut quality is even better than that of the 350 MPa cutting.

Fig. 8
figure 8

AWJ machined surface a 150 MPa single-pass cutting, b 150 MPa double-pass cutting, and c 350 MPa single-pass cutting

Specimens of run number 19 and the high-pressure control group were selected, and their surface morphology was measured using the NanoFocus μscan profiler as shown in Fig. 9, with a scanning frequency of 500 Hz and a resolution of 30 μm × 30 μm. As is demonstrated in Fig. 9a-c, the maximum height of the cutting surface in the Z-axis direction decreased from 118 to 98.4 µm by increasing the number of cuts, a reduction of 16.61%. Compared with the effect of high pressure cutting, the maximum height of 150 MPa double-pass cutting in the Z-axis direction is smaller than that of 350 MPa cutting.

Fig. 9
figure 9

Surface morphology produced by AWJ a 150 MPa single-pass cutting, b 150 MPa double-pass cutting, and c 350 MPa single-pass cutting

Figure 10 shows the comparison of experimental data between single-pass cutting, double-pass cutting, and the dotted line shows the cutting results of the 350 MPa control group. From Fig. 10a, it can be observed that double-pass cutting can greatly reduce the Ra of the cut surface by a maximum of 82.74% (Run Number 14) while narrowing the difference between the Ra of the cut surface with different cutting parameters. Compared to the control group with 350 MPa cutting, double-pass cutting at low pressure can achieve better experimental results than the control group based on all combinations of the selected cutting parameters. Figure 10b displays the resulting curve for Kt, where the double-pass cutting similarly reduces the Kt by up to 59.94% (Run Number 1) compared to the single-pass cutting. When compared with the control group cutting, the Kt in the double-pass cutting mode in the low-pressure condition is also smaller than the control group in both cases. Therefore, the cut quality obtained under 350 MPa waterjet can be achieved by using the double-pass cutting method in 150 MPa condition.

Fig. 10
figure 10

a Surface roughness and b kerf taper under different cutting strategies.

In this study, the same traverse speed is used in single-pass cutting and double-pass cutting, so the machining efficiency of double-pass cutting is reduced. However, under the same cutting time, the cutting quality is still better than that of single-pass cutting when the traverse speed of double-pass cutting is increased. Therefore, the double-pass cutting strategy under low pressure can prolong the service life of the equipment without reducing the machining efficiency.

4 Conclusions

Although increasing the waterjet pressure is an effective and much direct way to promote the cutting quality of AWJ, the manufacturing, maintenance, and safety of the ultra-high-pressure pump are suffering great challenges. In the present study, the method for achieving high waterjet cutting quality at a relatively low pressure of 150 MPa was experimentally explored, and the main conclusions are as follows:

  1. 1.

    The experimental results show that reducing the traverse speed and standoff distance significantly reduces the Ra and Kt. In addition, increasing the abrasive flow rate decreases the Ra, while an optimal abrasive flow rate exists for the Kt.

  2. 2.

    The cut quality at the relatively low pressure of 150 MPa can be improved by optimizing the process parameters. The highest quality appears when the traverse speed is 33 mm/min, the standoff distance is 0.66 mm, and the abrasive flow rate is 339 g/min, where the Ra and Kt are reduced by 6.03% and 86.67%, respectively.

  3. 3.

    Double-pass cutting with alternate directions is an effective strategy for improving the cut quality at the relatively low pressure. After double-pass cutting, the Ra has reduced by a maximum of 82.74% and the greatest reduction in Kt is about 59.94%. The surface quality exceeded that of the high pressure cutting.