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Article

Simulation and Experimental Study on Roll-Forming Limit of Cup

1
School of Materials Science and Engineering, North University of China, Taiyuan 030051, China
2
Engineering Research Center for Magnesium-Base Material Processing Technology, Ministry of Education of China, North University of China, Taiyuan 030051, China
*
Authors to whom correspondence should be addressed.
Materials 2022, 15(4), 1279; https://doi.org/10.3390/ma15041279
Submission received: 31 December 2021 / Revised: 7 February 2022 / Accepted: 7 February 2022 / Published: 9 February 2022
(This article belongs to the Special Issue Numerical and Experimental Investigations in Metal Forming)

Abstract

:
Roll forming can improve the material utilization rate and production efficiency of cups with a curved rotary profile, but there is no basis for the determination of forming limit. The DEFORM-3D software was used to simulate the roll forming of cups. The influence of the billet wall thickness and bottom thickness, coefficient of friction, radius of roller, and the fillet radius of the punch on the forming limit was studied, and the damage value and velocity vector were analyzed. The results showed that the forming limit of the billet’s wall thickness in roll forming for a cup is about 62%. With the increase of the ratio of the formed cup’s wall thickness to the billet’s bottom thickness, the forming limit of wall thickness will be slightly reduced. A larger radius of roller, fillet radius of punch, and friction coefficient between punch and billet and a smaller friction coefficient between roller and billet are good for decreasing the damage value and improving the roll-forming limit. According to the numerical simulation results, the roll-forming limit diagram of cups is established, and the accuracy of the forming limit diagram is verified by experiments.

1. Introduction

Cups with a curved rotary profile (as show in Figure 1) are common parts in industrial production. For example, in projectile bodies, drill pipe joints, etc., the final shape or a certain process in the forming process needs to be processed into a curved rotary profile [1,2,3,4,5]. This kind of part not only has extensive requirements, but also is produced in large quantities. In order to meet the requirements of high mechanical properties and mass production, cups with a curved rotary profile usually use the production process of machining after a cabbage, pierce and draw approach [6,7,8,9,10,11,12]. However, the material utilization rate is relatively low using this kind of production process for a cup with a curved rotary profile, and the longer the length of the part with smaller diameter, the lower the material utilization rate. Aiming at improving the material utilization rate, Xu Hengqiu et al., used the hot-spinning method to form the curved rotary profile of the cup and obtained good profile samples. However, the production efficiency of hot-spinning is low, which cannot meet the requirements of mass production, and it is very difficult to take out the mandrel from the workpiece after hot-spinning [13,14].
For the purpose of both meeting the requirements of mass production and increasing the material utilization rate of a cup with a curved rotary profile, a new technology, roll forming, was proposed on the basis of roll forging and drawing. The theory of roll forming is shown in Figure 2 [15,16,17,18,19,20,21,22,23]. During the process of roll forming, the punch is installed under the movable ram of the hydraulic press. The billet with the cup’s shape is pushed by the downwardly moving punch and makes the pre-forming rollers rotate. The curved rotary profile of the cup is formed by the specific groove shape on the surface of the rollers. During the roll-forming process, a thin flash may be formed at the gap between the rollers as part of the metal may flow into there, which will make it difficult for subsequent machining (as show in Figure 3). A triangular flash groove is designed between the adjacent pre-forming rollers so as to avoid the formation of a thin flash, and then the metal flows into the gap between the rollers and will form a triangular flash. The formed triangular flash can be eliminated by the shaping rollers, which are installed below the pre-forming rollers and rotated at an angle to the forming rollers (as shown in Figure 4). The influence of the triangular flash groove of pre-forming rollers on the quality of roll-formed parts has been studied and the optimized flash groove was put forward [15]. The influence of roller number on roll forming has been studied and the reasonable roller number for roll forming of a cup was suggested [16,17]. The forward slip of roll forming has been studied and the formula for roller design has been proposed [18,19]. The roll-forming process was compared with the traditional process from the aspects of material utilization, productivity, forming force, dies cost and subsequent machining time [20,21].
This method has successfully formed cups with a curved rotary profile [22,23], but there is no basis for determining the roll forming limit, which is one of the most important parameters to determine the forming process [24,25,26,27,28]. During the shaping of roll forming, only the triangular flash formed on the outer surface of the cup in the roll pre-forming is eliminated, and the deformation is small, so only the roll pre-forming limit needs to be studied. In this paper, the roll-forming limit of a cup is studied by means of numerical simulation and experiment. Three or four rollers can be used during the process of roll forming and the method of three rollers is used in this paper.

2. Numerical Simulation Model

DEFORM-3D finite element software is used for the numerical simulation analysis. In order to study the roll-forming limit efficiently, the roll forming roller is simplified into a groove with the same shape and size. The billet is regarded as a plastic body, the roller and punch are regarded as a rigid body, the material of the billet is pure aluminum 1060 and the material properties according to the supplier are shown in Table 1. The normalized Cockcroft and Latham fracture criterion is adopted [29,30]. According to the actual working conditions of roll forming, the friction coefficient between blank, roller and punch is set to 0.3, the billet’s and the ambient temperature are 20 °C, and the movement speed of the punch is 60 mm/s. The influence of the billet wall thickness and bottom thickness, coefficient of friction, radius of roller, and fillet radius of the punch on the forming limit is studied. The simplified numerical simulation model of roll forming is shown in Figure 5.

3. Simulation Results and Analysis

3.1. Effect of Billet’s Wall Thickness on Forming Limit

Numerical simulation of roll forming was carried out for five kinds of billets with bottom thickness (td) of 40 mm and wall thicknesses (t0) of 22, 26, 30, 34 and 38 mm, respectively. The wall thickness (t1) of the billet after forming was 13.5 mm. When the wall thickness of the billet is 22 mm to 34 mm, the damage value distribution of the formed part is shown in Figure 6. It can be seen from Figure 6 that the damage value is small, the shape of the formed part is good and no defects are found. However, with the increase of the billet’s wall thickness, the wall deformation increases, and the force required for the punch to push the bottom of the cup downward increases, resulting in the damage value increasing, the deformation of the fillet at the bottom of the billet’s shape and the enlargement of the fillet. The damage value distribution of the forming process is shown in Figure 7 when the wall thickness of the billet is 38 mm. It can be seen that due to the large deformation of the wall, the bottom of the workpiece shape is greatly deformed when the punch pushes the billet through the roller. With the downward movement of the punch, the workpiece deformation is mainly concentrated at the intersection of the bottom and the wall, resulting in the damage value increasing, the wall being thinned and the bottom and the wall being completely separated finally.

3.2. Effect of Billet’s Bottom Thickness on Forming Limit

Numerical simulation of roll forming was carried out for five kinds of billets with wall thickness (t0) of 34 mm and bottom thicknesses (td) of 10, 20, 30, 40 and 50 mm, respectively. The wall thickness (t1) of the billet after forming was 13.5 mm. The simulation results show that the roll forming of billets with bottom thicknesses of 30, 40 and 50 mm can be completed smoothly without defects or cracks. The metal flow velocity vector diagram during the forming process with a billet’s bottom thickness of 30 mm is shown in Figure 8. It can be seen that the bottom has sufficient strength to bear the deformation force of the billet wall when the wall thickness is nearly equal to the bottom thickness or the bottom thickness is thick, thus the roll forming can be carried out successfully.
When the bottom thickness of the billet is 20 mm, the forming process is nearly same as that in Figure 7, that is, the wall is thinned and fractured. When the bottom thickness of the billet is 10 mm, the metal flow velocity vector diagram during the forming process is shown in Figure 9. It can be seen from Figure 9 that the billet wall only has a small deformation at the intersection with the bottom and the deformation of the bottom is much greater than that of the wall when the punch pushes the bottom of the billet downward. This is caused by the deformation force needed by the billet wall being much greater than that the bottom can take as the bottom of the billet is too thin. The continuous movement of the punch finally resulted in the penetration of the billet bottom by the punch (punching off the billet bottom).

3.3. Establishing the Roll-Forming Limit

The above numerical simulation results show that the punch pushes the billet for active motion and the roller is passively driven by the billet during roll forming, but the roll wheel moves actively and the billet moves passively during roll forging, so the factors affecting the roll-forming limit are completely different from roll forging. The forming limit of roll forging depends on whether the billet can be bitten, but the forming limit of roll forming depends on whether the bottom of the workpiece can be penetrated (punched) or whether the wall can be thinned and fractured. When the bottom of the billet is thin and the wall deformation is large, the bottom of the workpiece will be penetrated as shown in Figure 9. When the bottom of the billet is thick and the wall deformation is too large, the problem of wall fracture after being thinned as shown in Figure 7 will occur. When the billet bottom is thick and the wall deformation is moderate, the roll forming can proceed successfully (as shown in Figure 6 and Figure 8). Orthogonal simulation is carried out for different wall thicknesses and the bottom thickness of the billet, and the results are shown in Table 2. The roll-forming limit diagram shown in Figure 10 can be obtained by Table 2. The abscissa in the figure is the ratio of the wall thickness of the formed cup to the bottom thickness of the billet (t1/td), and the ordinate is the deformation of the wall thickness ε:
ε = ( t 0 t 1 ) t 0 × 100 %
where t0 is the wall thickness of the billet before deformation and t1 is the wall thickness of the cup after deformation.
It can be seen from the forming limit diagram that when t1/td is less than 0.45, the wall thickness limit deformation that can make roll forming proceed successfully is about 62%. When t1/td is greater than 0.9, the wall thickness limit deformation of roll forming is about 52%. When t1/td is between 0.45 and 0.9, the deformation limit of wall thickness during roll forming decreases linearly with the increase of t1/td.

3.4. Effect of Friction Coefficient on Forming Limit

The effects of the friction coefficient between punch and billet (μ1) as well as roller and billet (μ2) on the forming limit are simulated according to the orthogonal method. The results are shown in Table 3, Figure 11 and Figure 12. According to Table 3, the influence diagram of the friction coefficient between punch and billet and the friction coefficient between roller and billet on the roll-forming limit can be obtained (as shown in Figure 13). It can be seen from Figure 11 to Figure 13 that damage value decreases and the roll-forming limit increases with the increase of the friction coefficient between the punch and the billet, which is mainly due to the increase of the friction coefficient being able to reduce the force of the punch acting on the bottom of the billet. The damage value increases and roll-forming limit decreases with the increasing friction coefficient between billet and roller, which is mainly due to the increase of the friction coefficient leading to the increase of metal flow resistance between rollers.

3.5. Effect of Roller Radius on Forming Limit

Different roller radiuses are simulated and the results are shown in Figure 14 and Table 4. It can be seen from Figure 14, when the roller radius is small and the damage value is large, that the cup’s wall is easily thinned and fractured. With the increasing roller radius, the damage value decreases and the cup’s wall is no longer stretched thin and fractured, and the roll forming can be carried out successfully. This is mainly due to the increasing roller radius being able to increase the contact area between the billet and the roller, which causes the increase of the friction force between the punch and the billet as well as the reduction of the axial tensile force of the billet wall.

3.6. Effect of Punch Fillet on Forming Limit

Different punch fillets are simulated and the results are shown in Figure 15 and Table 5. It can be seen from Figure 15 that the damage value is large and punching easily occurs at the bottom of the billet when the fillet radius of the punch is small. Increasing the punch fillet radius is conducive to the decreases in damage, the successful progress of roll forming and the improvement of the forming limit. This is mainly due to the small fillet radius of the punch easily producing large stress at the intersection of the cup’s billet wall and the bottom.

4. Experimental Verification

The formable point A and unformed point B near the forming limit (as shown in Figure 10) were experimentally verified on a hydraulic press with 1060 pure aluminum. At the points A and B, the billet wall thickness was 34 mm, and the bottom thicknesses were 30 and 20 mm, respectively. In order to keep the friction coefficient between roller and billet as well as billet and punch the same as 0.3 for the numerical simulation, no lubricant was used in the experiment. The other experimental parameters were consistent with the numerical simulation parameters. The billets and workpiece after roll forming are shown in Figure 16 and Figure 17. It can be seen that the experimental results are consistent with the numerical simulation results, indicating that the roll-forming limit diagram is feasible.

5. Conclusions

Based upon experimental and numerical results, the following conclusions are drawn:
  • When the bottom of the roll-forming billet is thin and the wall deformation is large, the bottom of the cup is penetrated. When the billet bottom is thick and the wall deformation is too large, the wall of the cup is thinned and fractured. When the billet bottom is thick and the wall deformation is moderate, the roll forming can proceed successfully.
  • The forming limit of the billet’s wall thickness in roll forming for a cup is about 62%. With the increase of the ratio of the formed cup’s wall thickness to the billet’s bottom thickness, the forming limit of wall thickness will be slightly reduced.
  • The increase of the friction coefficient between punch and billet or the decrease of the friction coefficient between roller and billet can decrease the damage value and improve the roll-forming limit.
  • Larger roller radius or punch fillet are good for decreasing damage value and the improvement of the roll-forming limit.
  • The reasonable control of process parameters, the bottom thickness of billet, the coefficient between punch and billet as well as billet and punch, the roller radius and the punch fillet, can all decrease the damage value and improve the roll-forming limit of a cup, that is, increase the wall deformation and reduce the forming process.
  • The roll-forming limit diagram of a cup was produced and the accuracy of the diagram was verified by experiments, which has important guiding significance for the actual roll-forming of cups.

Author Contributions

Conceptualization, B.Z., Y.D. and X.L.; numerical simulation, B.Z. and S.N.; experimental works, B.Z., X.L. and S.N.; writing—review and editing, B.Z., Z.W. and Y.Y. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by National Natural Science Foundation of China, grant number 51775519.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

The data supporting reported results are available on request from the corresponding author.

Conflicts of Interest

The authors declare no conflict of interest.

Abbreviations

Abbreviations, acronyms, and symbols
t0Wall thickness of billet
tdBottom thickness of billet
t1Wall thickness of deformed cup
μ1Friction coefficient between punch and billet
μ2Friction coefficient between roller and billet
RRadius of roller
rRadius of punch fillet
oRoll forming is successful
xRoll forming is unsuccessful

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Figure 1. Cup with curved rotary profile: (a) schematic diagram; (b) 3D model.
Figure 1. Cup with curved rotary profile: (a) schematic diagram; (b) 3D model.
Materials 15 01279 g001
Figure 2. Schematic diagram of roll forming.
Figure 2. Schematic diagram of roll forming.
Materials 15 01279 g002
Figure 3. Flash between rollers.
Figure 3. Flash between rollers.
Materials 15 01279 g003
Figure 4. Shaping during roll forming.
Figure 4. Shaping during roll forming.
Materials 15 01279 g004
Figure 5. Simulation of roll forming: (a) schematic diagram; (b) simulation model.
Figure 5. Simulation of roll forming: (a) schematic diagram; (b) simulation model.
Materials 15 01279 g005
Figure 6. Damage value distribution of roll formed cups by billets with different wall thicknesses of (a) 22 mm; (b) 26 mm; (c) 30 mm; (d) 34 mm.
Figure 6. Damage value distribution of roll formed cups by billets with different wall thicknesses of (a) 22 mm; (b) 26 mm; (c) 30 mm; (d) 34 mm.
Materials 15 01279 g006
Figure 7. Damage value distribution for forming process of billet with wall thickness of 38 mm. (a) Step of 90; (b) 105; (c) 135; (d) 153.
Figure 7. Damage value distribution for forming process of billet with wall thickness of 38 mm. (a) Step of 90; (b) 105; (c) 135; (d) 153.
Materials 15 01279 g007
Figure 8. Velocity vector of billet with bottom thickness of 30 mm. (a) Step of 5; (b) 30; (c) 65; (d) 203.
Figure 8. Velocity vector of billet with bottom thickness of 30 mm. (a) Step of 5; (b) 30; (c) 65; (d) 203.
Materials 15 01279 g008aMaterials 15 01279 g008b
Figure 9. Velocity vector of billet with bottom thickness of 10 mm. (a) Step of 5; (b) 30; (c) 39; (d) 42.
Figure 9. Velocity vector of billet with bottom thickness of 10 mm. (a) Step of 5; (b) 30; (c) 39; (d) 42.
Materials 15 01279 g009aMaterials 15 01279 g009b
Figure 10. Forming limit diagram of roll-forming for cups.
Figure 10. Forming limit diagram of roll-forming for cups.
Materials 15 01279 g010
Figure 11. Damage value distribution of different friction coefficients between punch and billet. (a) 0.01; (b) 0.1; (c) 0.3; (d) 0.5; (e) 0.7.
Figure 11. Damage value distribution of different friction coefficients between punch and billet. (a) 0.01; (b) 0.1; (c) 0.3; (d) 0.5; (e) 0.7.
Materials 15 01279 g011aMaterials 15 01279 g011b
Figure 12. Damage value distribution of different friction coefficient between roller and billet. (a) 0.01; (b) 0.1; (c) 0.3; (d) 0.5; (e) 0.7.
Figure 12. Damage value distribution of different friction coefficient between roller and billet. (a) 0.01; (b) 0.1; (c) 0.3; (d) 0.5; (e) 0.7.
Materials 15 01279 g012aMaterials 15 01279 g012b
Figure 13. Effect of friction coefficient on forming limit.
Figure 13. Effect of friction coefficient on forming limit.
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Figure 14. Damage value distribution of different roller radiuses of (a) 70 mm; (b) 75 mm; (c) 80 mm; (d) 85 mm; (e) 90 mm; (f) 95 mm.
Figure 14. Damage value distribution of different roller radiuses of (a) 70 mm; (b) 75 mm; (c) 80 mm; (d) 85 mm; (e) 90 mm; (f) 95 mm.
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Figure 15. Damage value distribution of different punch fillet radii of (a) 5 mm; (b) 10 mm; (c) 15 mm; (d) 20 mm; (e) 30 mm.
Figure 15. Damage value distribution of different punch fillet radii of (a) 5 mm; (b) 10 mm; (c) 15 mm; (d) 20 mm; (e) 30 mm.
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Figure 16. Billets for roll forming: (a) top view; (b) front view.
Figure 16. Billets for roll forming: (a) top view; (b) front view.
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Figure 17. Roll-formed cups: (a) bottom thickness of 20 mm; (b) 30 mm.
Figure 17. Roll-formed cups: (a) bottom thickness of 20 mm; (b) 30 mm.
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Table 1. Physical and mechanical properties of pure aluminum 1060.
Table 1. Physical and mechanical properties of pure aluminum 1060.
Yield Strength (MPa)Tensile Strength (MPa)Elongation (%)Hardness (HB)Elastic Modulus (GPa)Poisson’s Ratio
15602235690.3
Table 2. Orthogonal simulation results of different wall thicknesses and bottom thicknesses of the billet.
Table 2. Orthogonal simulation results of different wall thicknesses and bottom thicknesses of the billet.
No.t0 (mm)td (mm)μ1μ2R (mm)r (mm)Result
122100.30.39510
222120.30.39510
322150.30.39510
422200.30.39510
522300.30.39510
622400.30.39510
726100.30.39510
826120.30.39510
926150.30.39510
1026200.30.39510
1126300.30.39510
1226400.30.39510
1330100.30.39510×
1430120.30.39510×
1530150.30.39510×
1630200.30.39510
1730300.30.39510
1830400.30.39510
1934100.30.39510×
2034120.30.39510×
2134150.30.39510×
2234200.30.39510×
2334300.30.39510
2434400.30.39510
2538100.30.39510×
2638120.30.39510×
2738150.30.39510×
2838200.30.39510×
2938300.30.39510×
3038400.30.39510×
t0: wall thickness of billet; td: bottom thickness of billet; μ1: friction coefficient between punch and billet; μ2: friction coefficient between roller and billet; R: radius of roller; r: radius of punch fillet; o: roll forming is successful; x: roll forming is unsuccessful.
Table 3. Simulation results of different friction coefficients.
Table 3. Simulation results of different friction coefficients.
No.t0 (mm)td (mm)μ1μ2R (mm)r (mm)Result
138400.010.019510×
238400.10.019510×
338400.30.019510
438400.50.019510
538400.70.019510
638400.010.19510×
738400.10.19510×
838400.30.19510
938400.50.19510
1038400.70.19510
1138400.010.39510×
1238400.10.39510×
1338400.30.39510×
1438400.50.39510
1538400.70.39510
1638400.010.59510×
1738400.10.59510×
1838400.30.59510×
1938400.50.59510×
2038400.70.59510
2138400.010.79510×
2238400.10.79510×
2338400.30.79510×
2438400.50.79510×
2538400.70.79510
Table 4. Simulation results of different roller radiuses.
Table 4. Simulation results of different roller radiuses.
No.t0 (mm)td (mm)μ1μ2R (mm)r (mm)Result
138400.30.37010×
238400.30.37510×
338400.30.38010
438400.30.38510
538400.30.39010
638400.30.39510
Table 5. Simulation results of different punch fillet radii.
Table 5. Simulation results of different punch fillet radii.
No.t0 (mm)td (mm)μ1μ2R (mm)r (mm)Result
138400.30.3955×
238400.30.39510×
338400.30.39515
438400.30.39520
538400.30.39530
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Zhang, B.; Ning, S.; Wei, Z.; Duan, Y.; Li, X.; Yang, Y. Simulation and Experimental Study on Roll-Forming Limit of Cup. Materials 2022, 15, 1279. https://doi.org/10.3390/ma15041279

AMA Style

Zhang B, Ning S, Wei Z, Duan Y, Li X, Yang Y. Simulation and Experimental Study on Roll-Forming Limit of Cup. Materials. 2022; 15(4):1279. https://doi.org/10.3390/ma15041279

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Zhang, Baohong, Shengpeng Ning, Zeng Wei, Yali Duan, Xubin Li, and Yongbiao Yang. 2022. "Simulation and Experimental Study on Roll-Forming Limit of Cup" Materials 15, no. 4: 1279. https://doi.org/10.3390/ma15041279

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