Formability analysis
The forming angle is depicted in Fig. 9 as the angle α between the forming surface and the vertical direction in the process of NC incremental sheet forming. During the deformation process, shearing and stretching of the sheet material can produce thinning and fracture, the thickness change of the deformation region conforms to cosine law [25], as given in Eq. (1). When the forming angle α increases to a certain value that makes the deformation region rupture, then the limit value is called the forming limit angle (αmax), which can be used as an important index to measure the formability of sheet metal [26]. As the αmax increases, the deformation will be larger and the formability will be improved. In this experiment, the αmax was used as the standard of material formability.
The data table 5 recorded by the orthogonal experiment, A (spindle speed), B (step depth), C (tool diameter), αmax and T (forming temperature) were imported into SPSS data analysis software for the ANOVA, which the results are as shown in Table 6. The analyses were carried out with a 95% level of confidence. As a result, the value of P represents the confidence factor. If the value of P is less than 0.05, it is an important factor. The relevance is represented by the value of F. So the larger the value of F, the greater the influence of this factor on the αmax. According to the results, A (spindle speed), B (step depth), C (tool diameter) and their interaction have effects cataloging on the is A > B×C > B > C > A×B > A×C, the most significant factor is spindle speed A, then the step depth and tool diameter interaction B×C, other factors have little influence. It can be seen from the results that the increase of αmax with the enhancement of spindle speed. The formability of magnesium alloy increases sharply at 500rpm~2000rpm but does not change after 2000rpm. Compared with 500rpm, the formability has been greatly improved. Generally speaking, the formability increases with the increase of spindle speed, but the formability is basically unchanged when it reaches a certain speed. However, as the rotational speed increases, the temperature will continue to rise, resulting in ripple marks on the parts' exterior surfaces, making the surface quality very poor, as shown in Fig. 10. In addition, the αmax gradually decreases with the increase of step depth, but the change range is small. With the increase in tool diameter, the αmax only slightly increases, and the forming ability is slightly improved.
By analyzing the effect of processing parameters on forming ability and temperature, it can be concluded that the changing trend of forming ability is almost the same as that of temperature. With the increase of temperature, forming ability will be improved. However, the change of step depth on forming ability and temperature is the opposite. The main reason is that when the step depth increases in this range, the pressure of the sheet metal by the tool head will increase, which will increase the thinning rate, causing the sheet metal to crack, thus reducing the formability. At this point, the influence of pressure on the sheet metal is greater than that of temperature increase. The tool diameter has little influence on the formability. With the increase of tool diameter, the contact area between tool head and sheet the formability. With the increase of tool diameter, the contact area between tool head and sheet metal will be increased, resulting in an increase in temperature, thus improving the forming ability. Moreover, the smaller the diameter of the tool is, the more serious the sheet metal damage will be, and the poorer the formability will be.
Table 5 Experimental plan and results
Test no.
|
A (mm)
|
B (mm)
|
A×B
|
C (mm)
|
A×C
|
B×C
|
αmax (°)
|
T (℃)
|
1
|
500
|
1.0
|
3
|
12
|
3
|
1
|
29
|
52
|
2
|
500
|
2.0
|
1
|
8
|
1
|
2
|
23
|
61
|
3
|
500
|
1.5
|
2
|
16
|
2
|
3
|
27
|
60
|
4
|
1000
|
1.0
|
1
|
12
|
1
|
1
|
36
|
87
|
5
|
1000
|
2.0
|
2
|
8
|
2
|
2
|
41
|
90
|
6
|
1000
|
1.5
|
3
|
16
|
3
|
3
|
33
|
110
|
7
|
1500
|
1.5
|
2
|
12
|
1
|
1
|
59
|
80
|
8
|
1500
|
1.0
|
3
|
8
|
2
|
2
|
47
|
100
|
9
|
1500
|
2.0
|
1
|
16
|
3
|
3
|
56
|
112
|
10
|
2000
|
2.0
|
2
|
16
|
3
|
1
|
71
|
140
|
11
|
2000
|
1.5
|
3
|
12
|
1
|
2
|
62
|
110
|
12
|
2000
|
1.0
|
1
|
8
|
2
|
3
|
49
|
95
|
13
|
2500
|
2.0
|
3
|
12
|
2
|
1
|
59
|
120
|
14
|
2500
|
1.5
|
1
|
8
|
3
|
2
|
51
|
100
|
15
|
2500
|
1.0
|
2
|
16
|
1
|
3
|
55
|
120
|
16
|
3000
|
1.5
|
1
|
8
|
2
|
1
|
64
|
130
|
17
|
3000
|
1.0
|
2
|
16
|
3
|
2
|
65
|
125
|
18
|
3000
|
2.0
|
3
|
12
|
1
|
3
|
52
|
135
|
Table 6 ANOVA results of αmax
Factor
|
Mean average error
|
Degree of freedom
|
F value
|
Sig value
|
Significance
|
A
|
560.633
|
5
|
21.425
|
0.045
|
Significant
|
B
|
33.500
|
2
|
1.280
|
0.439
|
|
C
|
32.000
|
2
|
1.223
|
0.450
|
|
A×B
|
4.081
|
2
|
0.156
|
0.865
|
|
B×C
|
80.082
|
2
|
3.061
|
0.246
|
|
A×C
|
0.333
|
2
|
0.013
|
0.987
|
|
Dimensional accuracy analysis
To intuitively comprehend the deformation characteristics and thickness distribution at each FHISF stage, contour maps of the cross-sectional CAD model and the digital model of the part were extracted from CATIA for comparison, as shown in Fig. 11. Due to the symmetry of the parts, only the half-part outline was discussed, which is "+" when the parts are above the CAD model and "-" at the bottom. The edge areas of the part bent to varying degrees in each period, which was caused by the clamping plate. Due to the lack of backing support, the load applied during the initial forming step caused bending in the sheet. This is mostly determined by the distance between the clamping edge and the tool's contact location. There is no obvious upper and lower corner in the initial forming stage of the sidewall region, where the main occurrence is bending deformation. It was found that there are obvious convex marks in the lower corner at various forming stages, which are left by the tool during the last lap. The tool squeezes the metal, causing it to flow to the side edge and accumulate at the undeformed area, increasing the thickness of this section. The part's bottom is uneven all around, with the center position being higher than the edge position. Because the bottom edge location is subjected to more downward pressure from the tool during the process of local plastic deformation, the bottom center position is always higher than the tool processing position throughout the machining process.
Thickness distribution in FHISF
Comparing simulated thickness results with actual results, as shown in Fig. 12, it could be found that the thickness of the sidewall region is not uniform in the early forming stage. At the intermediate and final forming stages, the thickness of the sidewall region is generally homogeneous at around 0.99mm, which is 11% thinner than the theoretical thickness. This is because friction heating necessitates rotational contact between the tool and the sheet, making it impossible to use 100% of the material, and a part of the materials in the deformation area is extruded to the bulge at the bottom. The massive thickness decrease identified during experimental investigation in the corner region was also found in simulated components. Fig. 13 exhibits the profile thickness distribution of the half part. In the unformed area, the sheet metal thickness did not change around 1.60mm, and the sheet metal thickness near the upper corner area decreased rapidly. In the sidewall area, the thickness of the sheet metal gradually reached a stable state as the tool descended, and was distributed around the theoretical thickness. It was found that the part's sidewall region did not attain a stable thickness at first, but reached the minimum thickness after a specific forming depth which was found during experimental investigation to be about 16mm (Fig. 14). The results show that the designed simulation model can accurately predict the thinning trend and can be used as a further reference for effective stress and strain.
Stress and strain distribution in FHISF
The stress and strain levels throughout the FHISF stages are extremely difficult to determine owing to the nature and complexity of the process. Therefore, Mises stresses and plastic strain were analyzed by the FEM. Fig. 15 illustrates the stress-strain evolution of HFISF stages. As the forming stage develops, the stress and strain values increase. The maximum stress value for the early forming stage is 165.1 MPa, 171.1 MPa for the intermediate stage, and up to 174.2 MPa at the final forming stage. The part's maximum strain is 0.437 in the early forming stage, whereas the plastic strain increases but does not vary significantly in the intermediate and final forming stages, both around 0.471. The plastic strain increased from the early to the intermediate stage, but it did not much change from the intermediate to the final stage. The plastic strain value reached its maximum value when forming the sidewall area, and the thickness of the sidewall area was almost unchanged. So the trend of stress and strain in the part is very similar during each forming stage.