numerical and experimental validation for sheet metal hydroforming
Transcription
numerical and experimental validation for sheet metal hydroforming
NUMERICAL AND EXPERIMENTAL VALIDATION FOR SHEET METAL HYDROFORMING PROCESS RULES Antonio Del Prete, Alfredo Anglani, Teresa Primo, Barbara Manisi University of Salento, Department of Engineering of Innovation ABSTRACT A research program, whose objective is to understand the influence and the management of the process variables in sheet metal hydroforming, is developed [1]. The main project objective is to demonstrated how it is possible to orient the process designer choices in the n-dimensions process space, where n is the number of its variables. The present work illustrates the results obtained trying to define the best practise rules for sheet metal hydroforming. Keywords: sheet hydroforming, CAE, process rules definition. 1. INTRODUCTION Nowadays, hydroforming techniques are largely accepted by industries for the production of components characterized by good surface quality, high-dimensional accuracy together with high drawing ratio and complex shapes [1-6]. The main distinction among the large variety of hydroforming techniques is usually based on the used raw material: tubular or sheet material. Today the tubular material is predominantly used for the mass production; actually sheet hydroforming is used for small batch production because both its cycle time and clamping forces (large tooling investments) are higher than the tube hydroforming ones [7]. However, sheet hydroforming process offers several advantages over tube Hydroforming [8]. Furthermore, conventional sheet metal forming techniques reach their limits in certain cases. Optimized application of dies and presses for sheet hydroforming leads to a reduction of product specific costs and thus to lower costs per part. This is extremely important for low volume productions. As generally known, there are great differences between conventional deep drawing and sheet hydroforming, mainly due to the usage of a pressurized liquid as forming tool. This leads to a frictionless force transmission to the sheet and to a high contact pressure between sheet and die. This results in nearly no friction between blank and fluid and high friction forces between rigid punch and blank when deep drawing is realized with counter pressure. Higher forming forces can be transferred to the forming zone, having as a result greater draw ratios (parts with a higher drawing height). In this specific case, a “shape factors” set is defined in order to orient the designer within the process design space for metal components produced through the application of sheet hydroforming. These shape factors are used to track the process performances through their variation thanks to the usage of the numerical simulation which is later validated with an appropriate experimental activity. Basically, it is possible to distinguish three factors typologies which constitute the main variables of the hydroforming process: - geometries (tool radius, presence of redrawing); - materials (thickness, physical and mechanical properties); - equipment calibration (fluid pressure, blankholder force, friction, etc). These three groups of factors are correlated but their relationships are not known. For this reason the establishment of rules which give the chance to verify their influence on the process performance can be considered a valid support tool in the process design definition phase. In this paperwork the authors’ attention is con- centrated on the influence of factors such as: geometric parameters and material characteristics on the process quality. The correlation among process variables, shape factors described below and quality process indexes is investigated. 2. REFERENCE MODELS AND SHAPE FACTORS DEFINITION Different geometric models, MODi (with i = 1,…, 5), significant for the automotive component class taken into account, are defined. Two representative models, MOD1 and MOD5, are taken into account in this work [9]. Having as reference the chosen models, the shape factors are defined to have adimensional coefficients representative for the given geometries. is quite common to have a redrawing height as geometric characteristic. For this type of components two different shape factors are defined, Rh and Rc, by the equations (2) and (3), respectively. Rh = L2 / Hc (2) where L2 has already defined, and Hc is indicated in Figure 2. Rc = Lc / Hc (3) where Lc and Hc are, respectively, the maximum dimension in top view and the maximum depth of a given redrawing area (Figure 2). Figure 2. MOD5 Punch numerical model: shape factors definition. Figure 1. Typical FE model for numerical simulation of MOD1 with indication of L2 and the main punch dimension. Considering L2, the smallest dimension of the initial blank (Figure 1), and Himb as the drawing depth, the first shape factor R2 is defined by the ratio: R2 = L2 / Himb (1) The numerical and experimental analysis campaigns are characterized by the same initial blank. For this reason the variability of R2 is due only to the different considered drawing depths. For industrial products, for example a metal formed panel for fuel tanks construction, it The L2 value, for the MOD1, is equal to 670 mm, this means that low R2 values correspond to high drawing depths. For MOD5, L2 is equal to 683 mm and punch radius is equal to 10 mm. The maximum reached drawing depth is equal to 150 mm for all the considered models. The commercial finite element explicit code LS-Dyna is used for the numerical simulations. The tooling such as: punch, fluid chamber and upper and lower blankholders were created through the usage of rigid materials formulation (*MAT_20 in LS-Dyna), while anisotropic material formulation (*MAT_37 in LS-Dyna) was used for the blank. Considered tests are related to numerical simulation made using a low carbon steel blank (FeP04) and aluminium alloy Al6061 with defined characteristics (Table 1 and and Table 2). HyperMesh® and HyperView® are used for pre and post processing phases. Table 1. FeP04 Material Properties used in the simulation. σ y (MPa) R E (GPa) ν n 195.5 0.3 179 1.9 0.19 An example of the obtained relationships by different combinations of thicknesses and material types for the considered model MOD1 is reported below (Figure 6). The obtained process responses refer to a geometric model with the following characteristics: a punch radius is equal to 50 mm and a die radius is equal to 20 mm. Table 2. Al6061 Material Properties, used in the simulation. σ y (MPa) R E (GPa) ν n 72 0.3 255 1.9 0.09 Two initial blank thickness values are adopted for numerical and experimental simulation: 0.7 mm and 1 mm. For all the considered configurations a common value is used for friction (µ=0,125). Through the usage of the *AIRBAG CARD, with linear fluid option of LsDyna, is defined the fluid pressure in FE model. The blankholder force is a load applied to a rigid body. The optimal definition of the blankholder force and fluid pressure time-dependent characteristics is obtained through a sequence of numerical tests with the application of a trial and error method. 3. PROCESS PLOT CHARTS The numerical simulation results allow to understand the dependency of some process performance indexes (e.i. percentage thickness reduction, FLD map at the end of the forming phase, etc.) on the defined shape factors. Specific plot charts are developed to summarize these relationships. 3.1 Influence of the defined shape factors on the percentage thickness reduction Thanks to the results obtained from the numerical simulation of the considered models it is possible to define the necessary plot charts. As first step, the maximum thickness reduction (in percentage) is considered as quality process index response depending on the defined shape factors. Figure 3. MOD1, first plot chart typology referred to the considered geometric configuration for different material types and initial sheet thicknesses. The obtained plot is divided in two areas: the lower one with thickness percentage reduction (tpr) less than 30% can be considered the process feasibility window, the upper one with output values higher than 30% can be considered the process unfeasibility window. In models definition M1 or M5 stand for Model type MOD1 or MOD5, Fe or Al stand for considered material type, 1 or 07 stand for considered thicknesses, 50_20 stand for punch and die radius respectively. The feasibility window is then defined by the analytical expression: tpr < 30%. For R2>9 it is possible to observe that the aluminium alloy and the low carbon steel models have the same trend. In particular, for R2≥9 the obtained characteristics have a trend parallel to the x-axis expressing a low sensitivity compared with R2. For R2<9 the obtained characteristics are strictly dependent on the considered material. In particular, for R2<9 both materials present an increase in tpr. This increase has a higher gradient in the case of the aluminium alloy. Both the considered mate- rials have an increase of the tpr gradient when lower values of initial blank thickness are examined. The tpr process response is investigated for different R2 values varying punch and die radius in the case of the most promising material (low carbon steel). The obtained results are shown in Figure 4, where all the considered cases are included in the feasibility window (maximum tpr < 30%). Figure 4. MOD1, First plot chart typology in the case of: different punch and die radius for the same material and initial blank thickness. In detail, the tpr characteristic for M1_Fe1_10_10 with punch and die radius both equal to 10 mm it does not show any dependency on the R2 factor. This means that the most critic aspect ( the process unfeasibility reason ) is due to the punch radius value. In fact, the tpr of the model with the same punch radius value (10 mm) but die radius equal to 20 mm (M1_Fe1_10_20) shows a low dependency on R2. The two models with punch radius equal to 50 mm, instead, have similar trend of tpr and they both show a dependency on the R2 factor. In detail, the model with die radius equal to 10 mm (M1_Fe1_50_10) shows two main significant variations of the tpr gradient, when R2 is equal to 16 and 7. On the contrary, the model with die radius equal to 20 mm (M1_Fe1_50_20) shows two main significant variations of the tpr gradient when R2 is equal to 13 and 7,5. Then an increase of 100% of die radius leads to a minimum and a maximum tpr reduction of 1% and of 3.8% respectively. On the contrary, an increase of punch radius of 400% involves a minimum tpr reduction of 11.2% and a maximum of 12.2% greater than the one which can be obtained with a die radius variations. In order to consider the presence of a geometric variation like a redrawing height, Rc and Rh factors are investigated (Figure 9). For this plot the initial blank thickness is equal to 1 mm and a low carbon steel is the considered material. The punch radius for MOD5 is equal to 25 mm and die radius is equal to 10 mm. Figure 5. First plot chart typology for MOD5 for different considered values of the shape factors Rc and Rh. The plot shows that only for Rc > 10.5 it is possible to have feasible configurations for MOD5 and only for Hc equal to 20 mm or 25 mm. Furthermore, the three curves have similar trend and they overlap each other for Rc > 9,5. The better solution is when Rh factor is equal to 34, then the quality index decreases in correspondence of an increase of this shape factor. When Rh factor is equal to 27, there is feasibility only for Rc > 11, while when Rh factor is equal to 23, there is not feasibility for any of the investigated cases. 3.2 Influence of the defined shape factors on the Forming Limit Curve Distance response In this case the used approach is different by the one used for the other plot charts definitions. In fact, in the previous cases a scalar process response is considered (tpr). It is well know that metal forming process quality can be monitored thanks to the Forming Limit Diagram (FLD) analysis which gives a general overview of the material deformation states. In this case, an alternative plot chart typology can be considered reducing to a scalar value the general process response overview given by the FLD. As scalar process response, the distance between the highest deformation state of the part on the FLD and the correspondent limit state given by the Forming Limit Curve, is considered for the different tested conditions. This is a defined value: Forming Limit Curve distance (FLCd). The FLCd variation in relation to the R2 shape factor variation for different material types and blank thicknesses for a given geometry (MOD1) leads to the third plot chart typology definition (Figure 12) Figure 6. Third plot chart typology for MOD1 considering different combinations given by different material types and blank thicknesses for the same geometry. The above reported shows plot the same results included in Figure 3 but referred to a different performance index. For aluminium alloy, the FLCd plot shows a more critical situation than tpr, for initial thickness equal to 0.7 mm. This is due to the different behaviour of the aluminium in comparison with the one obtained for the steel. In fact for low carbon steel the two plots are in accordance showing that there is feasibility for all the investigated shape factors. In the case of the aluminium alloy, instead, the models with initial thickness equal to 1 mm show feasibility, with tpr index, and fracture for R2 equal to 8 when the FLCd index is considered. Furthermore for the models with initial thickness equal to 0.7 mm plot it is evident a fracture condition for R2 equal to 6, with tpr index, and R2 equal to 9.5 with FLCd index. This kind of plot chart is very difficult to obtain because of when different blank thicknesses are considered the specific FLD are needed. On the obtained diagram, a positive FLCd value stands for feasible conditions while a negative one stands for an unfeasible condition characterized by a situation where some areas of the formed parts the deformation states are higher than the maximum ones allowable by the FLC for the given material type and thickness. 4. NUMERICAL EXPERIMENTAL CORRELATION All the produced plot charts are based on an extensive numerical simulation campaign. For this reason, in order to verify what is numerically obtained, appropriate experimental tests are needed. Thanks to the developed experimental test rig, hydroformed parts are obtained with the process set up studied in the numerical simulation phase. The comparison between numerical and experimental parts are made thanks to the thickness values monitored on the formed parts and compared with the ones obtained with the numerical simulations. As reference, two of the many studied cases are reported below. In the first case the hydroformed part MOD1 made by low carbon steel with an initial blank thickness of 1.0 mm in the case of a punch radius equal to 50 mm and a die radius equal to 10 mm is compared with its numerical simulation results. The experimental and numerical thicknesses values measured along three directions (x, y and along a generic section A-A, Figure 10) are compared. As it can be appreciated, thanks to the reported data, (Figure 7 – Figure 9) there is a uniform thickness distribution and a good agreement between numerical and experimental values with a discordance of about 4%. Figure 7. numerical-experimental thickness values comparison for MOD1, along X-X section. Figure 8. numerical-experimental thickness values comparison for MOD1, along Y-Y section. Figure 9. numerical-experimental thickness values comparison for MOD1, along A-A section. Figure 10 reports the thicknesses map obtained thanks to the numerical simulation and the areas where the experimental data are measured, while Figure 11 shows the real hydroformed component. Figure 11. experimental component MOD1. The second comparison case is related to the MOD5 model where the examined configuration is the one made by low carbon steel, blank thickness equal to 0.7 mm, Hc=20 mm, L=65 mm (Figure 2), punch and die radius of 10 mm. Figure 12-Figure 14 report the comparison between numerical and experimental thickness values for MOD 5. It is evident a uniform thickness distribution, and a better agreement between numerical and experimental value with a discordance of about 2.8 %. Figure 12. Numerical-experimental thickness values comparison for MOD5, along X-X section. Figure 13. Numerical-experimental thickness values comparison for MOD5, along Y-Y section. Figure 10. thickness map of numerical simulation for MOD1. Figure 14. numerical-experimental thickness values comparison for MOD5, along A-A section. Figure 15 reports the thicknesses map obtained thanks to the numerical simulation and the areas where the experimental data are taken. Figure 16 shows the real component. Figure 17. numerical-experimental thickness values comparison for MOD5, along X-X section. Figure 18. Numerical-experimental thickness values comparison for MOD5, along Y-Y section. Figure 15. numerical simulation thickness map for MOD1. Figure 16. experimental component MOD5. Finally, to evaluate the repetitiveness of the measured thickness values, experimental data are measured along X and Y direction on five different hydroformed components in the case of the MOD5 geometry and the obtained data have been compared as it is reported in Figure 17 and 18. From the reported data it can be assumed a good correlation and a very good repetitiveness. 5. CONCLUSION The obtained results allow to say that a first step ahead has been done in order to define possible orientation instruments in the process design space for sheet metal hydroforming. Useful suggestions can be obtained by such a kind of process plot chart in a preliminary process design review. The presented activity has to be completed by industrial test cases which can give useful feedbacks to the presented methodology. However, it is evident how an extensive numerical and experimental activity is needed to develop useful process plot charts and to define quality indexes for different material types. Through a first analysis of shape factors is possible to establish the rules of design process upstream of numerical simulation of hydroforming process. ACKNOWLEDGEMENTS Authors are very grateful to “MUR: Ministero dell’Università e della Ricerca” for funding this work recognized as I.T.Idro: innovative solutions for sheet hydroforming. Special thanks are addressed to Stamec srl which has the role of industrial partner of the project. LIST OF REFERENCE 1. Zhou L. X., Lang L. H., Danckert J., Zhang S. H., Nielsen K. B., “Research on the effect of the local constraints on sheet hydroforming with the movable die”, Numisheet Conference 2005, vol. A, pp. 532-537. 2. Sokolowski T., Gerke K., Ahmetoglu M., Altan T., “Evaluation of tube formability and material characteristics: hydraulic bulge testing of tubes”, Journal of Materials Processing Technology 98, 2000, pp. 34–40. 3. Rimkus W., Bauer H., Mihsein M.J.A., “Design of load-curves for hydroforming applications”, Journal of Materials Processing Technology 108, 2000, pp. 97–105. 4. Carleer B., Van der Kevie G., De Winter L., Van Veldhuizen B., “Analysis of the effect of material properties on the hydroforming process of tubes”, Journal of Materials Processing Technology 104, 2000, pp. 158–166. 5. Siegert K., Haussermann M., Loesch B., Rieger R., “Recent developments in hydroforming technology”, Journal of Materials Processing Technology 98, 2000, pp. 251-258. 6. Zhang S. H., Wang Z. R., Xua Y., Wang Z. T., Zhou L. X., “Recent developments in sheet hydroforming technology”, Journal of Materials Processing Technology 151, 2004, pp. 237-241. 7. Ch. Hartl, “Research and advances in fundamentals and industrial applications of hydroforming”, Journal of Materials Processing Technology 167, 2005, pp. 383-392. 8. Lang L., Danckert J., Nielsen K. B., Zhou X., “Investigations into the forming of a complex cup locally constrained by a round die based on an innovative hydro mechanical deep drawing method”, Journal of Materials Processing Technology 167, 2005, pp. 191-200. 9. Del Prete Antonio, Primo Teresa, Papadia Gabriele, Manisi Barbara, “Process Rules for Sheet Metal Hydroforming”, ISC 5th International Simulation Conference, Delft, The Netherlands, EUROSIS publication, 2007, pp. 109-113. 10. Lihui Lang, Joachim Danckert, Karl Brian Nielsen, “Investigation into effect of pre-bulging during hydromechanical deep drawing with uniform pressure onto the blank”, International Journal of Machine Tools & Manufacture 44, 2004, pp. 649-657.