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Abstract

In the deep drawing process, achieving a higher drawing ratio has always been considered by researchers. In this study, a new concept of hydrodynamic deep drawing with two consecutive stages without additional operations such as annealing is proposed to increase the limit drawing ratio of the cups. The effective parameters were investigated numerically and experimentally in the forming of Al1200 cylindrical cups. At first, the desired value of punch diameter ratio was determined based on finite element simulation results and was utilized to increase the cup formability. Next, the effects of pressure paths on the cup thickness, separation, and rupture were studied in each forming stage. The cup formability was investigated based on a new proposed framework to obtain the maximum possible limiting drawing ratio, and the desired conditions were determined. Finally, a cup was formed with a high drawing ratio of 3.4 which was a good achievement in comparison with the literature.

Keywords

Aluminum alloy two-stage hydrodynamic deep drawing finite element simulation pressure path drawing ratio

Introduction

The sheet hydroforming process has a wide range of applications in automotive, aerospace, etc, and has many advantages over conventional deep drawing.^1–5 In recent years, hydrodynamic deep drawing assisted by radial pressure (HDDRP) has given good results in the forming of parts with a higher limit drawing ratio. In HDDRP, the blank is formed on the surface of the punch by the pressurized liquid in the die cavity. Meanwhile, the liquid flows out dynamically which leads to a uniform pressure on the blank outer edge. Many other advantages are obtained by using this process, such as high dimensional accuracy, good surface quality, and production of complicated parts.^2,6

Lang et al.² investigated the forming of Al6016-T4 aluminum alloy in the HDDRP process experimentally. They studied and predicted the fracture and wrinkling of cylindrical cups. Finally, they formed the cylindrical cup with the maximum drawing ratio of 2.46 from a 1.15 mm thick sheet. Hashemi et al.⁷ investigated the HDDRP forming of conical parts numerically and experimentally. They determined the process window diagrams (PWDs) to compare Al1050/St14 laminated sheet and its constituent single layers. They redefined the limiting drawing ratio (LDR) of a conical cup in three forms depending on cone angle, tip radius, and cup height to investigate the effects of those parameters under similar conditions. They obtained various values of drawing ratios for different LDR definitions from 3.12 to 9.9. Hashemi et al.⁸ developed a new optimization procedure by an adaptive combination of simulated annealing optimization algorithm and finite element method to predict the optimal pressure load in hydrodynamic deep drawing (HDD) of bilayer composite cups. Salahshoor et al.⁹ investigated the effects of several HDDRP parameters on punch force and thickness distribution of pure copper cylindrical cups with a drawing ratio of 1.9 numerically and experimentally. Khademi et al.¹⁰ modified the HDDRP with inward flowing liquid. Also, they studied the effect of controlling radial pressure and the cavity pressure on thickness distribution numerically and experimentally. Bhatt and Buch¹¹ developed an expert system to design a die for multi-stage deep drawing (MSDD) operations to improve quality and productivity. Pourkamali et al.¹² studied the MSDD of an industrial part with annealing between steps. Zhu et al.¹³ proposed the multi-stage HDD to form a stainless-steel cup with complex stepped geometries. They stated that it is difficult to manufacture the part in a single HDD stroke due to the large unsupported areas of the blank between the punch and the die and also the small corner radius which can lead to wrinkling and tearing. So, the elimination of the defects needed a multi-stage HDD process. They investigated the effect of pre-form depth on the final products and could obtain a drawing ratio of 4 with a 0.4 mm thick stainless steel sheet. Li et al.¹⁴ put forward a multi-stage HDD process to study the precision of deep conical parts. They stated that forming a desired conical part with a single deep drawing process is difficult due to the large deformation and the high drawing ratio. Also, they explained that the control of defects such as wrinkling and tearing in the multi-stage HDD process is difficult contrary to the single HDD process. Thus, it is crucial to investigate the defect pattern and parameters interaction for controlling the forming quality. Accordingly, they examined the sequential deformation of a conical part using theoretical and numerical analyses and experiments. They formed a conical part with a drawing ratio of 3.7 from the 2024O aluminum alloy sheet with a thickness of 1 mm.

In the deep drawing process, getting a higher drawing ratio as well as less production time with the desired quality has been always considered by researchers. Oluwole et al.¹⁵ investigated the drawing ratio in conventional deep drawing of fully annealed Al1200 sheets with different thicknesses of 0.6–2 mm. They formed a cylindrical cup with a maximum drawing ratio of 1.87 for 1.55 mm sheet thickness. Li et al.¹⁴ formed a conical 2024-O aluminum cup from an initial blank with 1.0 mm thickness and 96.5 mm diameter with a maximum drawing ratio of 3.7. Zhang et al.¹⁶ were able to reach a drawing ratio of 2.5 and 2.6 for Al1100 and mild steel (A-K steel) cups, respectively from 1 mm thick blanks using the hydromechanical deep drawing. Lang et al.¹⁷ formed cylindrical cups with the maximum drawing ratios of 2.46 and 3.11 for a 1.15 mm thick Al6016-T4 and a 1.24 mm thick Al1050-H0, respectively by hydromechanical deep drawing.

In this study, a novel two-stage hydrodynamic deep drawing process (TS-HDD) based on the HDDRP process in only one die set was utilized to achieve a higher drawing ratio. It is worth noting that the forming of a similar cup by a conventional deep drawing process requires an increase in the number of forming stages in several separate dies. Also, in most cases, additional operations such as annealing or redrawing are required between successive stages. The proposed TS-HDD design in this research improved the limiting drawing ratio using only one die set in two consecutive stages without additional operations. This will cause a reduction of production time and tooling cost compared to the conventional deep drawing process. The most important feature of this new design is the use of only one die set with two coaxial punches and a stepped pressure chamber instead of several separate dies. This feature reduces the number of drawing stages compared to the conventional deep drawing and causes a consecutive forming without moving the part between different dies. Therefore, it is crucial to investigate the defects and the process parameters to achieve a high-quality part with a high drawing ratio. So, the effects of parameters on rupture and thickness distribution have been discussed in the TS-HDD using FE simulations and experimental tests.

Material and methods

In this research, first, a method for determining the appropriate diameter ratio of the punches was studied. Then, the desired pressure paths and maximum values at each stage were investigated separately. A new framework was proposed considering a two-stage consecutive process to determine the obtainable maximum drawing ratio in TS-HDD. Finally, a cylindrical cup was formed with a high “drawing ratio” and high “height to diameter ratio” by the TS-HDD process under the desired working conditions obtained from investigations.

A 1.5 mm thick Al1200 sheet fully annealed at 350°C for 120 min was used. Round blanks were cut from aluminum sheets. Standard tensile tests according to ASTM-E8M were performed at three rolling directions of 0°, 45°, and 90° to obtain the mechanical properties. The material properties and the true stress-strain curve of the material obtained from the tensile tests are given in Table 1 and Figure 1, respectively.

Table 1.

Mechanical and physical properties of Al1200 sheet.

Parameter	Value
Yielding stress (MPa)	39
Elongation (%)	41
Young’s modulus (GPa)	69
Density (kg/m³)	2710
Poisson’s ratio	0.3
Strain hardening exponent, n	0.33
Strength coefficient, k (MPa)	162.28

Figure 1.

Stress-strain curve of Al1200.

Figure 2(a) shows a schematic of the TS-HDD process and the die parametric dimensions. The main components consist of two coaxial punches (primary and secondary), metal blocks, a blank holder, and a stepped pressure chamber. Based on the nature of the hydrodynamic process, no sealing is used in the process. In the TS-HDD for each stage, the oil leaks out dynamically from the contact surface of the blank holder and the die. The interface between the die and blank holder was ground metal contact and no o-ring was used for sealing in the die (region g in Figure 2(a)). In stage one, the leaking liquid creates pressure under the blank and around its rim at the same time as in the HDDRP process. In stage two, the hydrodynamic process occurs by small leakage of liquid from the blank holder/die interface like the first stage, but the pressure is created on the outside and the edge of the pre-formed cup. Also, an initial pressure of 2 MPa was exerted before the movement of the punches at each forming stage. The SAE 20/5.6 cSt hydraulic oil was used in the experiments. Figure 2(b) shows the assembled TS-HDD die set installed on the press machine. The experiments were performed using a 150 kN hydraulic press.

Figure 2.

(a) Schematic of TS-HDD process and die parametric dimensions and (b) assembled TS-HDD die installed on the press.

Figure 3 schematically illustrates the forming stages of the TS-HDD process. In stage one, the pre-formed cup is produced by moving the primary and secondary punches in the vertical direction simultaneously, and the oil leakage from the grounded blank holder/die interface causes the pressure around the blank outer edge. In stage two, by removing the cylindrical block and fixing the primary punch on the blank holder, the final cup is formed by moving down the secondary punch. Also, there is low oil leakage from the blank holder/die interface, which creates pressure on the wall and edge of the pre-formed cup. In each stage, the pressure in the die cavity is increased to the maximum value adjusted by the pressure control valve. The blank holder does not apply any force on the sheet independently. In the second stage, the primary punch plays the blank holder role for the pre-formed cup, which is constrained with the main blank holder and also exerts no force on the pre-formed cup. It should be noted that the forming stages are performed consecutively. So, the pre-formed cup is not removed between the first and second stages and no additional operations such as annealing are performed. This is an essential feature of the TS-HDD process in this study.

Figure 3.

Schematic of: (a) stage one; forming of the pre-formed cup and (b) stage two; forming of the final cup.

To evaluate the anisotropy behavior at a given angle θ to the rolling direction, the plastic strain ratio (r-value) is calculated using the following equations,¹⁸

r_{θ} = \frac{ε_{w}}{ε_{t}}

(1)

where $ε_{w}$ and $ε_{t}$ are the width and thickness strains, respectively, measured in a uniaxial tension specimen cut at an angle (θ) to the rolling direction. Since it is difficult to measure the thickness strain for thin sheets with sufficient precision, it can be concluded from assuming the volume constancy¹⁸ as follows:

r_{θ} = \frac{- ε_{w}}{ε_{1} + ε_{w}}

(2)

where $ε_{1} = \frac{l}{l_{0}}$ and $ε_{w} = \frac{w}{w_{0}}$ . Therefore,

r_{θ} = \frac{\ln [\frac{w}{w_{0}}]}{\ln [\frac{w_{0} l_{0}}{wl}]}

(3)

On the other hand, to apply sheet anisotropy in finite element simulation, the yield stress ratios (R values) must be introduced as¹⁹:

R_{11} = \frac{σ_{11}}{\bar{σ}}, R_{22} = \frac{σ_{22}}{\bar{σ}}, R_{33} = \frac{σ_{33}}{\bar{σ}}, R_{12} = \frac{σ_{12}}{\bar{σ}}

(4)

where $σ_{11}$ , $σ_{12}$ , and $σ_{22}$ are the yield stresses at 0°, 45°, 90° to the rolling direction, respectively. $σ_{33}$ is the yield stress at thickness orientation and $\bar{σ} = σ_{11}$ is the yield stress at 0° direction.

Subsequently, plastic stress ratios can be obtained by equations (5)–(7) with assuming $R_{11} = R_{13} = R_{23} = 1$ .¹⁹ So, the plastic strain ratios (r values) are obtained from the experimental tests while the yield stress ratios (R values) of the aluminum sheet shown in Table 2 are acquired by equations (5)–(7).

R_{22} = \sqrt{\frac{r_{90} (r_{0} + 1)}{r_{0} (r_{90} + 1)}}

(5)

R_{33} = \sqrt{\frac{r_{90} (r_{0} + 1)}{r_{0} + r_{90}}}

(6)

R_{12} = \sqrt{\frac{3 r_{90} (r_{0} + 1)}{2 (r_{45} + 1) (r_{0} + r_{90})}}

(7)

Table 2.

Plastic strain ratios (r values) and yield stress ratios (R values) for Al1200.

Thickness (mm)	r ₀	r ₄₅	r ₉₀	R ₁₁, R₁₃, R₂₃	R ₂₂	R ₃₃	R ₁₂
1.5	1.707	1.075	1.434	1	0.966	1.111	1.084

The explicit finite element analysis was used to simulate the process by ABAQUS 6.12. The Hill yield criterion was used to assign anisotropic yielding.¹⁹ Three-dimensional models were used for the tooling and the blank. Figure 4 shows the FE model of the die for the TS-HDD process. Only one-quarter of the 3D model was used because of structural symmetry and reducing the computation time. C3D8R 8-noded solid linear brick element was used for meshing the blank. Four elements along the thickness were meshed based on the convergence of the maximum punch force. For meshing the die rigid model, a four-node shell element R3D4 was applied. The pressure chamber and the blank holder were entirely fixed while the punches were defined to move in the vertical direction. Fluid pressure constraints were exerted under the blank surface and also on the outer edge of the blank. According to Figure 2(a), the gap between the pressure chamber and the blank holder (G) was exerted and fixed. The velocity of both punches was 20 mm/s. The multiplication factor of 100 was applied in the simulation.²⁰ At stage two, the primary punch was fixed as a blank holder of the pre-formed cup and the secondary punch moved down with the constant velocity. The whole process was performed in four steps, that is, two steps in each stage; Step one, applying the pre-bulging pressure, and step two, loading the fluid pressure in the pressure chamber. Coulomb friction model was used to define the contact frictions. Coefficients of frictions of 0.14 and 0.04 were used at the punch-blank and other interfaces, respectively.^6–8 The Hollomon’s power law equation of $σ = K ε^{n}$ was applied to state the flow stress in the simulation.

Figure 4.

Finite element model of the die set.

The maximum thinning was considered as a fracture criterion which was calculated by equation (8).

maximum thining (%) = \frac{t_{0} - t_{f}}{t_{0}} \times 100

(8)

Where $t_{0}$ and $t_{f}$ are the initial blank and cup thicknesses, respectively.^6,8

The thickness of the formed cup in the finite element simulations is calculated by measuring the distance between the nodes on the inner surface and the nodes on the outer surface of the blank. Figure 5 schematically shows the method of measuring the thickness of a formed cup by finite element simulation and the corresponding thickness distribution. In this study, the maximum thinning percentage of 41% was obtained, which means rupture occurs if the thickness of the aluminum part in simulations becomes <0.885 ≃ 0.89 mm, and the forming process fails. This value was in close agreement with those measured experimentally.

Figure 5.

Schematic of measuring cup thickness in the finite element model.

Results and discussions

Punch diameter ratio (PDR)

In TS-HDD, the diameter of the preformed cup is determined by the diameter of the primary punch, and its height is determined by the limit drawing ratio of the first stage and the diameter of the primary punch. Meanwhile, it is necessary to determine the desired ratio between the diameter of the primary and secondary punches to get the higher total drawing ratio. So, to investigate a criterion for evaluating the degree of formability, the ratio of the primary punch diameter ( $D_{PP}$ ) to the secondary punch diameter ( $D_{SP}$ ) is defined by equation (9).

Punch Diameter Ratio : PDR = \frac{D_{PP}}{D_{SP}}

(9)

The PDR is approximately equal to the drawing ratio of the second stage. The limiting drawing ratio of stage one ( $β_{0}$ ) and the limiting redrawing ratio ( $β_{n}$ ) are obtained from equations (10) and (11), respectively:

β_{0} = \frac{D}{d_{0}}

(10)

β_{n} = \frac{d_{n - 1}}{d_{n}} n = 1, 2, 3, . . .,

(11)

where D is the initial blank diameter, $d_{0}$ is the diameter of the formed cup in the first stage (pre-formed cup), $d_{n - 1}$ and $d_{n}$ are the cup diameters at (n−1)th and (n)th stages, respectively.

In this study, the diameter of the secondary punch is constantly equal to 35 mm, so it is necessary to determine the desired primary punch diameter to obtain the desired PDR. A higher amount of PDR makes it difficult to form the final cup and may lead to rupture. On the other hand, lowering the amount of PDR may cause severe thinning or tearing of the pre-forming cup. Therefore, determining the desired PDR can lead to the production of a sound part with a high drawing ratio.

Based on previous studies on the conventional drawing process, the “diameter reduction percentage” according to equations (12)–(14) and “height-to-diameter ratio” according to equations (15)–(17) are used for determining and comparing the formability at each stage:

R_{t} = 1 - (1 - R_{0}) (1 - R_{1})

(12)

% R_{0} = 100 \times \frac{D - d_{0}}{D}

(13)

% R_{1} = 100 \times \frac{d_{0} - d}{d_{0}}

(14)

where $R_{t}$ is the total percent reduction in diameter, $% R_{0}$ and $% R_{1}$ are the percentages of diameter reduction in stages one and two, respectively, and $d$ is the cup diameter in the second stage.

H R_{1} = \frac{h_{1}}{D}

(15)

H R_{2} = \frac{h_{2}}{d_{0}}

(16)

H R_{t} = \frac{h_{2}}{D}

(17)

where $H R_{t}$ is the total height-to-diameter ratio related to the final cup, $H R_{1}$ and $H R_{2}$ are the height-to-diameter ratios in stages one and two, respectively, and $h_{1}$ and $h_{2}$ are the heights of the pre-formed and final cups, respectively.

Because the maximum possible drawing ratio of the pre-formed cup in the first stage may not result in the best thickness distribution of the final cup and it may even increase the risk of rupture in the second stage, FE simulations were performed for different initial blank diameters of 85, 90, and 95 mm and different primary punch diameters with a constant tip radius of 7 mm to determine the desired drawing ratio. Then, the minimum thicknesses at the critical region of final cups (zone B) were compared as shown in Figure 6(a). The constant maximum pressure of 10 MPa for both stages was applied. As shown in Figure 6(a), the lowest percentage of thickness variation ratio (TVR%) for three different total drawing ratios shows the same results as occurred with the primary punch diameter of 54 mm.

Figure 6.

Thickness variation ratio of critical area B: (a) versus different primary punch diameter, and versus different tip radius in primary punch diameter of, (b) 54 mm, (c) 51 mm, (d) 57 mm, and (e) 60 mm.

In the following, to evaluate the effect of the primary punch radius and determine the desired value, experiments were performed by several optional radii for different primary punches diameters and the results were compared (Figure 6(b)–(e)). According to the two-stage die design, for a certain diameter of the primary punch, the maximum size of the punch radius is about the maximum radial distance between the primary and secondary punches’ radii. Therefore, due to the constant diameter of the secondary punch, the maximum applicable radius for the primary punch will also increase with increasing the diameter of the primary punch.

As shown in Figure 6(b) to (e), the thickness variation ratios of the critical region corresponding to the final cup are reduced with an increasing radius of the primary punch tip. Also, it can be seen for all cases that the effect of the tip radius on critical thickness will increase with increasing the diameter of the initial blank, as shown by ATVR%. Also, as shown in zone Z in Figure 6(b), in addition to reducing the amount of thickness variation ratio for the maximum radius (9 mm), the differences between the TVR% of various blanks have been reduced too. This can be seen in almost all other cases too (Figure 6(c)–(e)). Comparing the results shown in Figure 6, it can be seen that despite the increase in maximum tip radius in punches 57 and 60 mm and subsequently decrease in TVR%, the minimum TVR% is related to the radius 9 mm of the primary punch with the diameter of 54 mm. So, according to the results and what was discussed, the primary punch diameter of 54 mm and the radius of 9 mm were considered as the desired values. Due to the constant diameter of the secondary punch (35 mm) and based on equation (9), the desired PDR value was obtained 1.54. So, based on equation (13), the desired $% R_{0}$ for blanks 85, 90, and 95 mm are equal to 36%, 40%, and 43%, respectively. Based on equation (14), $% R_{1}$ corresponding to the second stage of the TS-HDD process for all blanks with different diameters is 35%.

Table 3 shows the TS-HDD die dimensions shown in Figure 2(a). Dimensions of the die and the primary punch were considered based on the results discussed above.

Table 3.

TS-HDD die dimensions corresponding to Figure 2(a).

Parameter	Value (mm)
Primary punch diameter, DPP	54
Secondary punch diameter, DSP	35
Blank holder inside diameter, DBH	54.1
Primary die inside diameter, DPD	58.5
Secondary die inside diameter, DSD	39
Primary punch tip radius, r_PP	9
Secondary punch tip radius, r_SP	6
Primary die entrance radius, r_PD	5
Secondary die entrance radius, r_SD	8
Gap between die and blank holder, G	1.7

Forming pressure paths

In the hydroforming process, the pressure loading path affects the part thickness distribution as an important parameter. Since the hydrodynamic process is performed in two consecutive stages, the desired pressure path for each stage should be investigated separately. The basis of the pressure path in this research which applied for each stage was according to paths $P_{1},$ $P_{2}$ , and $P_{3}$ shown in Figure 7(a); $P_{1} :$ the pre-bulging path $(P_{1} = 2 MPa)$ , $P_{2} :$ the linear path corresponding to punch speed which was considered 20 mm/s, and $P_{3} :$ the final path which the oil leaks out from the pressure relief valve during this path. Different paths were examined based on the critical thickness of cups to determine the desired pressure path at each stage. Figure 7 shows the desired pressure paths used in the simulations and experiments in stages one and two. To determine the desired maximum pressure at each forming stage ( $P_{\max 1}$ and $P_{\max 2}$ ), pressure paths with a different maximum value of 5–30 MPa were investigated.

Figure 7 .

Pressure paths corresponding to different $P_{max}$ in a) Stage 1 and b) Stage 2.

To determine the best pressure path, the variation curves of the thickness decrease in area B of the cylindrical cup were compared at different maximum pressure. Figure 8 shows the thickness decrease curves in area B of the pre-formed and the final cups related to different pressure paths in simulation and experimental tests. It can be seen in Figure 8(a), as the final pressure increases, the decrease in thickness also increases with an almost constant gradient. Also, at the final pressure of near 5 MPa and less, bursting occurred on the radius of the deformed cup. Figure 9(a) illustrates the deformed part in which bursting occurred because of the low level of pressure in the forming stage one. For the maximum pressure between 5 and 10 MPa, the separation defect occurred at the contact area of the pre-formed cup wall with the primary punch. At pressures higher than 10 MPa, the thickness reduction increased with slight fluctuation. Therefore, although higher maximum pressure eliminates the separation defect, it was caused an increase in the thickness reduction and also the punch force. Therefore, the lowest final pressure that resulted in a non-defective part was considered as the desired pressure in stage one.

Figure 8.

Thickness decrease curve for area B at different maximum pressures: (a) the pre-formed cup and (b) the final cup.

Figure 9.

Defective workpieces: (a) the pre-forming stage, $P_{\max}$ = 4 MPa and (b) the final stage, $P_{\max}$ = 19 MPa.

Also, as shown in Figure 8(b), the results for the final cup show that at final pressures lower than 7.5 MPa the thickness decrease was reduced. At maximum pressures higher than 7.5 MPa, the thickness decrease was increased again with a steep gradient. And finally, for the pressures more than 17.5 MPa, tearing occurred in the critical region. Figure 9 indicates the defective part in which the higher level of pressure has caused the bursting of the workpiece at the end of forming stage two.

So, according to the results, considering the pressure paths associated with the least thinning, pressure paths with the maximum value of 10 and 5 MPa were considered as the desired pressure paths of the primary and secondary forming stage, respectively. Figure 10 shows the thickness distribution curve and final aluminum cup formed with a high drawing ratio by these pressure paths (paths A and C in Figure 7). The critical zone is B where the highest reduction in thickness occurred. Furthermore, it is worth mentioning that the maximum prediction error of thickness distribution is 5%, which is due to the error accumulation and the material work hardening at the primary stage.

Figure 10.

Final cylindrical cup and thickness distribution curve corresponding to the paths with $P_{\max 1}$ = 10 MPa and $P_{\max 2}$ = 5 MPa.

Maximum drawing ratio (MDR)

To determine the maximum possible total drawing ratio ( $MD R_{t}$ ) of the aluminum cup in the TS-HDD process, the final cup formability based on the maximum drawing ratio of the first stage ( $MD R_{1}$ ) was investigated by the framework presented in Figure 11. In the first step, according to Figure 12 for stage one of the TS-HDD process, the minimum final pressure versus the drawing ratio is investigated using FE simulation. As shown in this figure, by increasing the diameter of the initial blank, the minimum final pressure is also increased. On the other hand, as the pressure rises, the drawing ratio increases to a certain value. According to the results, the maximum initial blank diameter of 127 mm (DR = 2.35) was achieved to form the aluminum pre-formed cup. The cup was not formed at any pressure for diameters higher than this. In step 2, based on the results obtained from Section 3.2, the lowest maximum pressure which led to a part without defect for all drawing ratios could be investigated as an option of desirable maximum pressure in stage one ( $P_{\max 1}$ ). In step 3, to determine the desired maximum pressure at the second stage ( $P_{\max 2}$ ), simulations were performed at different maximum pressures considering the obtainable $MD R_{1}$ with the desired $P_{\max 1}$ obtained from the previous steps. In the case of the non-formability of the final cup in step 3 for the selected $MD R_{1}$ , the next drawing ratio was examined as the maximum value. Therefore, as shown in step 4, a lower drawing ratio was examined as the next possible $MD R_{1}$ . For example, the first option to check the final cup formability is the highest drawing ratio (with BD = 127 mm) of Figure 12. If the final cup is not fully formed with this drawing ratio, the next option (with BD = 126 mm) is considered as the maximum drawing ratio.

Figure 11.

Framework to determine maximum drawing ratio in TS-HDD process.

Figure 12.

The drawing ratio corresponding to maximum pressure in stage one of TS-HDD.

According to the results, the $MD R_{1}$ which led to the production of the final cup without defect was obtained 2.2 (BD = 119 mm shown in Figure 12), which corresponds to the maximum pressure of 12.5 MPa (path B in Figure 6(a)). Also, to determine the desired $P_{\max 2}$ in step 3, the simulation of different pressure paths (as shown in Figure 7(b)) under the desired conditions of stage one ( $P_{\max 1}$ = 12.5 MPa and $MD R_{1}$ = 2.2) was examined. By investigating the results, the lowest critical thickness reduction of the final cup occurred at the $P_{\max 2}$ of 7.5 MPa (path D in Figure 7(b)).

Figure 13 shows the simulation and experimental pre-formed cup corresponding to the $MD R_{1}$ of 2.2 and the pressure path with a maximum value of 12.5 MPa. As can be seen, there is a slight bulge at the bottom of the cup that occurred in the gap between the secondary punch radius and the interior edge of the primary punch due to the nature of the TS-HDD die design. This bulge increases the contact surface of the secondary punch with the blank and helps the formability of the final cup at the beginning of the second stage. Figure 14 shows the FE simulation and experimental final aluminum cylindrical cup by TS-HDD process with a high total drawing ratio ( $MD R_{t}$ ) of 3.4 which was obtained under the desired conditions presented in Table 4.

Figure 13.

The pre-formed cup corresponds to the path with a final pressure of 12.5 MPa.

Figure 14.

The final cup corresponds to the path with a final pressure of 7.5 MPa.

Table 4.

The desired working and geometrical conditions of cups in TS-HDD.

Parameter	Pre-forming stage (stage 1)	Final forming stage (stage 2)	TS-HDD (total value)
Desired maximum pressure (MPa)	12.5	7.5 MPa	–
Pre-bulging pressure, P₀ (MPa)	2	2	–
Percentage of diameter reduction	$% R_{0}$ = 54.6%	$R_{1}$ = 35.1%	$R_{t}$ = 70.6%
Maximum drawing ratio (MDR)	$MD R_{1}$ = 2.2	$MD R_{2}$ = 1.54	$MD R_{t}$ = 3.4
Blank diameter (mm)	119	≃56	–
Formed cup height (mm)	$h_{1}$ ≃ 59	$h_{2}$ ≃ 98	–
Height to diameter ratio (HR)	$H R_{1}$ = 0.49	$H R_{2}$ = 1.75	$H R_{t}$ = 0.82

Figure 15 indicates the thickness distribution of the final formed cup with the maximum drawing ratio. The precision of the numerical model along the A-B-C direction was validated by the experiment. The highest decrease in thickness occurred in the radius of the final cup (critical zone B). Also, there is a slight local thinning in the cup wall area which occurred due to bending and unbending in the tip radius area of the pre-formed cup. The maximum prediction error of thickness distribution is 5%, which is attributed again to the error accumulation and also the effect of material work hardening during the process.

Figure 15.

Thickness distribution curve of the final cup with the maximum drawing ratio.

As it was discussed, a cylindrical Al1200 cup was formed with a high drawing ratio of 3.4 and $H R_{t}$ of 0.82 using the proposed TS-HDD process by applying the desired conditions at each forming stage.

Conclusion

In this research, a two-stage hydrodynamic deep drawing (TS-HDD) was proposed as a new design of the HDD process. To study the process efficiency, the effects of process parameters on thinning and rupture of aluminum Al1200 cylindrical cups were discussed by experiments and FE simulations.

The punch diameter ratio (PDR) and the primary punch tip radius were investigated by FE simulations. The PDR of 1.54 and the punch tip radius of 9 mm were obtained as the desired values which led to the smallest thinning percentage at the final cup critical area.

Then, the effects of pressure paths on cups thickness were examined for a specified initial blank diameter. It was concluded that rupture, separation defects, or critical thinning occurred in the lower final pressure. The separation defect was eliminated by increasing the maximum pressure, but higher maximum pressure led to higher thinning and tearing in the critical area. Therefore, in both forming stages, the pressure paths with the lowest maximum value that produced a sound part were considered as the desired pressure paths ( $P_{\max 1}$ = 10 MPa and $P_{\max 2}$ = 5 MPa).

Finally, the maximum possible total drawing ratio ( $MD R_{t}$ ) in the TS-HDD process was examined based on a new proposed framework in four steps. According to the results, the $MD R_{1}$ and the desired $P_{\max 1}$ and $P_{\max 2}$ which resulted in the maximum total drawing ratio in the TS-HDD process were obtained 2.2, 12.5, and 7.5 MPa, respectively. Therefore, in this study, by improving the formability of an aluminum alloy compared to other deep drawing processes, the cylindrical aluminum cup was formed with a very high total drawing ratio of 3.4 numerically and experimentally using two consecutive stages in only one die set without additional operations.

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) received no financial support for the research, authorship, and/or publication of this article.

ORCID iDs

S H Alavi Hashemi

S M H Seyedkashi

References

Koc

Hydroforming for advanced manufacturing. 1st ed. New York, NY: Elsevier, 2008.

Lang

Danckert

Nielsen

KB.

Investigation into hydrodynamic deep drawing assisted by radial pressure part I, experimental observations of the forming process of aluminum alloy. J Mater Process Technol 2004; 148: 119–131.

Jalil

Hoseinpour Gollo

Seyedkashi

SH.

Process analysis of hydrodynamic deep drawing of cone cups assisted by radial pressure. Proc IMechE, Part B: J Engineering Manufacture 2017; 231(10): 1793–1802.

Fazlollahi

Morovvati

Mollaei Dariani

Theoretical, numerical and experimental investigation of hydro-mechanical deep drawing of steel/polymer/steel sandwich sheets. Proc IMechE, Part B: J Engineering Manufacture 2019; 233(5): 1529–1546.

Pan

Investigation on deformation behavior of magnesium alloy sheet AZ31B in pulsating hydroforming. Proc IMechE, Part B: J Engineering Manufacture 2021; 235(1–2): 198–206.

Gorji

Alavi-Hashemi

Bakhshi-jooybari

, et al. Investigation of hydrodynamic deep drawing for conical–cylindrical cups. Int J Adv Manuf Technol 2011; 56: 915–927.

Hashemi

Hoseinpour Gollo

Seyedkashi

SMH

. Study of Al/St laminated sheet and constituent layers in radial pressure-assisted hydrodynamic deep drawing. Mater Manuf Process 2017; 32(1): 54–61.

Hashemi

Hoseinpour Gollo

Seyedkashi

SMH

, et al. A new simulation-based metaheuristic approach in optimization of bilayer composite sheet hydroforming. J Braz Soc Mech Sci Eng 2017; 39: 4011–4020.

Salahshoor

Gorji

Bakhshi-Jooybari

Analysis of the effects of tool and process parameters in hydrodynamic deep drawing assisted by radial pressure. J Braz Soc Mech Sci Eng 2019; 41: 145.

10.

Khademi

Sadegh yazdi

Bakhshi-Jooybari

, et al. Investigation of a modified hydrodynamic deep drawing assisted by radial pressure with inward flowing liquid process. MATEC Web Conf 2018; 190: 09003.

11.

Bhatt

Buch

SH.

An expert system of die design for multi stage deep drawing process. Procedia Eng 2017; 173: 1650–1657.

12.

Pourkamali

Shahabizadeh

Babaee

Finite element simulation of multi-stage deep drawing processes & comparison with experimental results. Int J Mech Aerosp Ind Mechatron Manuf Eng 2012; 6(1): 217–221.

13.

Zhu

Wan

Zhou

, et al. Investigation into influence of pre-forming depth on multi-stage hydrodynamic deep drawing of thin-wall cups with stepped geometries. Adv Mater Res 2012; 457–458: 1219–1222.

14.

Meng

Wang

, et al. Effect of pre-forming and pressure path on deformation behavior in multi-pass hydrodynamic deep drawing process. Int J Mech Sci 2017; 121: 171–180.

15.

Oluwole

Anyaeche

Faola

OV.

Effect of draw ratio and sheet thickness on earing and drawability of Al 1200 cups. J Miner Mater Char Eng 2010; 9(5): 461–470.

16.

Zhang

Jensen

Danckert

, et al. Analysis of the hydromechanical deep drawing of cylindrical cups. J Mater Process Technol 2000; 103(3): 367–373.

17.

Lang

Danckert

Nielsen

KB.

Investigation into the effect of pre-bulging during hydromechanical deep drawing with uniform pressure onto the blank. Int J Mach Tools Manuf 2004; 44(6): 649–657.

18.

Marciniak

Duncan

SJ.

Mechanics of sheet metal forming. Oxford: Butterworth Heinemann, 2002.

19.

ABAQUS 6.12. Documentation, user’s manual. Providence, RI: Dassault Systèmes Simulia Corp, 2012.

20.

Lang

Danckert

Nielsen

KB.

Investigation into hydrodynamic deep drawing assisted by radial pressure part II. Numerical analysis of the drawing mechanism and the process parameters. J Mater Process Technol 2005; 166: 150–161.

Investigation of consecutive two-stage hydrodynamic deep drawing of aluminum cylindrical cups

Abstract

Keywords

Introduction

Material and methods

Results and discussions

Punch diameter ratio (PDR)

Forming pressure paths

Maximum drawing ratio (MDR)

Conclusion

Footnotes

Declaration of conflicting interests

Funding

ORCID iDs

References