J. Cent. South Univ. (2014) 21: 493−499 DOI: 10.1007/s1177101419668 New type of groove used to improve friction in roll forging JIA Zhi(贾智) , ZHOU Jie(周杰), JI Jinjin(姬金金) School of Materials Science and Engineering, Chongqing University, Chongqing 400044, China © Central South University Press and SpringerVerlag Berlin Heidelberg 2014 Abstract: A FEM model for a failed industrial example of roll forging was established to analyze the generation mechanisms of the mismatch of size and shape of two spring board. To demonstrate the formulation of these defects, the bites condition and contact status between rectangular groove and workpiece during rolling the first and second spring boards were analyzed. Then, a new ovaldiamond groove combining oval groove and diamond groove was presented to eliminate these defects. By analyzing field variables under the same deformation degree, the larger friction can be obtained on the contact surface of workpiece and the ovaldiamond groove. The physical experiment validates that the ovaldiamond groove can eliminate these defects effectively, and the size of part is in good agreement with design requirement. Key words: roll forging; spring board; ovaldiamond groove; rectangular groove; automobile front axles 1 Introduction Roll forging is a process for reducing the crosssectional area of heated bars or billets by passing them between two driven rolls that rotate in opposite directions and have one or more matching grooves in each roll. Compared to other conventional forming processes, the roll forging possess has remarkable advantages, such as greater productivity, greater material utilization ratio, better product quality, more simple equipment structure, longer life of rolling dies, an improved environment and automation and lower production costs. For a successful roll forging process, it is necessary to consider the roll separation force, the spread, the elongation, and the appropriate geometry of the roll groove. A lot of factors, such as metal flow, stresses, rollingseparation force, temperature and elastic deflection of the rolls, must be taken into account [1−2]. Several publications in the literature analyzed the forming mechanism with physical testing and numerical simulation theory. KNAPINSKI [3] found that the roll geometry underwent considerable distortion over the whole roll length during rolling, and this would result in incorrect dimensions of the finished product. BENASCIUTTI et al [4] proposed a simplified approach to computate thermal stresses in work roll of hot rolling mills, and found that the largest thermal gradient developed within a small region close to work roll surface. YOO et al [5] presented an analytical model to predict the surface profile of a workpiece in a roundto2R oval groove and a square sectionto2R oval groove rolling sequence, and found that the surface profile of the workpiece in the 2R oval groove is smaller than that of the 1R oval groove [5]. The effects of the penetration rate of rolling tool on the fatigue strength and the residual stress of grooverolled products were investigated by KIM et al [6]. BYON et al [7] studied the effect of roll gap adjustment on the exit cross sectional area variation of workpiece in a twostand groove rolling process, and found that the previous stand has a more strong influence on this area of workpiece than the next stand. TIAN et al [8] developed a new rolling force model and a torque model to analyze the rolling pressure in asymmetrical rolling process, and found that the length of cross shear region increases with the increase in the speed ratio. Many researchers have paid attentions to roll forging and studied the groove design and die parameters. NA et al [9] presented a design method of forming groovetoseparating groove rolling sequence used in slit rolling process. SHAHANI et al [10] studied the temperature distribution, stress, strain and strain rate field in the roll die, and used the artificial neural network to predict the behavior of the slab during the hot rolling process. The wear resistance of hot rolling was evaluated on the basis of a tribological test aimed at reproducing the damage mechanisms by PELLIZZARI et al [11]. Not only shaft parts but also billets for precision die forging can be produced through roll forging. Hence, this Foundation item: Project(51275543) supported by the National Natural Science Foundation of China; Project(cstc2009aa30121) supported by the Key Program of Chongqing Science and Technology Foundation, China Received date: 2012−09−24; Accepted date: 2013−11−10 Corresponding author: JIA Zhi, PhD Candidate; Tel: +86−13996399957; Email: [email protected] 494 process has been applied widely. SEDIGHI and MAHMOODI [12] studied the precision roll forging process of compressor blade, and the effect of elastic behavior of the machine structure as well as rolls deflection on the material flow and roll separating force. The blankmaking roll forging die of front axle, premolding roll forging die and final forming roll forging die were designed respectively by LI et al [13]. ERVASTI and STAHLBERG [14] facilitated the development of adequately shaped grooves in the reducer rolling mill so that the flash volume obtained in production was reduced during forging process of automobile front axles. CAI [15] studied the forming process of automobile front axles, and the rolling die was designed. Because the material deformation styles during roll forging are different from die forging, there are some defects during roll process, and the design of rolling groove is very difficult. With the development of computers, the design of roll forging process has been optimized with the implementation of interactive graphics programs and simulation methods based on finite elements analysis. In this work, a complicated industrial example with defects was analyzed, and the experiments and FEM analysis were adopted to research the generation mechanisms of defects in roll forging. A new type of groove (ovaldiamond groove) was presented to overcome the defects, such as the mismatch and undersize of two spring board. The field variable was analyzed to explain the difference between ovaldiamond groove and rectangular groove. Finally, the physical experiment was carried out to validate the feasibility of this research. J. Cent. South Univ. (2014) 21: 493−499 Fig. 2 Automobile front axle after finishing roll forging 1) The shape of two spring board is mismatched. 2) A fold is located in spring board. 3) Size cannot meet the design requirements. After many times of trial, it was found that these defects changed during the forging process, and firstly appeared at the second step roll. So it could be supposed that these defects appeared because of the unreasonable design of the first and second step rolls, as shown in Fig. 3. The firststep roll was used to initially distribute material for each characteristic segment of the part, and an adequate longitudinal distribution of metal was obtained after this step. The secondstep roll was designed to provide an approximate shape of spring board for final operation, and the fold and undersize were aroused by unreasonable design of the secondstep roll. So, the mismatch of two spring board was originated from the firststep roll, and the fold was attributed to the secondstep roll. 2 Failed industrial example In this section, a complicated roll forging example was presented, in which the rolled forging was used to prepare the billets for forming the automobile front axles. The technological process of roll forging for a front axle is given in Fig. 1. However, it failed in industrial application because of some defects located in spring board. The defects are summarized below, and shown in Fig. 2. Fig. 1 Technological process of forming of automobile front axle Fig. 3 Failure workpiece after roll forging: (a) After firststep roll; (b) After secondstep roll To resolve these defects, it is needed to design reasonable die groove for spring board of the firststep and secondstep rolls. In this failed industrial application, the crosssections of the grooves are rectangular in firststep dies, and “hatshaped” in the secondstep die, as shown in Fig. 4. In this work, more attention has been paid on firststep dies. Firstly, it is needed to analyze the forming mechanism of these defects. But in actual production, field variables like strain and stress are very difficult to test, and it is very luxury using physical research method J. Cent. South Univ. (2014) 21: 493−499 495 Fig. 4 Crosssection of groove at firststep and secondstep roll (Unit: mm): (a) Rectangular groove; (b) Hatshaped groove to optimize these variables. Fortunately, the finite element method has been accurate enough to substitute the physical research method. 3 FEM analysis for failed industrial example 3.1 FEM model In order to further understand the formation mechanism of the defects, finite element method was employed to simulate the roll forging process. One of the primary advantages of finite element analysis is its ability to parametrically analyze the forming process which is difficult to obtain experimentally. Design of roll forging die is very complicated owing to the varied surface and multiple segments of the die. The parametric design has been realized using the UG6.0 software for reducing the time of model building. Dies designed in UG can be directly imported into the finite element software by the interface between them. The analysis of the roll forging process adopts the rigidplastic FEM based on the flow formulation of the penalized form of the incompressibility. In this work, the workpiece material is AISI 5140, and the material flow behavior is determined by the flow stress data. The true stress−strain curves used in this simulation is presented in Fig. 5. In this twostep roll forging process, constant shear friction model is used for the bulkforming simulation. Fig. 5 Stress−strain curves of AISI 5140: (a) At 800 °C; (b) At 1000 °C; (c) At 1200 °C In order to reduce CPU time and eliminate the effect of irrelevant factors, the following assumptions are developed: 1) The dies are defined as rigid bodies, and the billet is plastic material. 2) The friction factor on the material/die interface is constant. The shear friction model is used in this simulation, and it states that the friction is a function of the yield stress of the deforming body. 3) The rotational velocity of roller is constant during the rolling process. 4) The material is isotropic and the yielding behavior follows the Von Mises yield criterion. 5) The mesh type of the billet is tetrahedral. The rectangularhat groove system model for roll 496 J. Cent. South Univ. (2014) 21: 493−499 forging is shown in Fig. 6, and the model consists of a part and two dies. The workpiece is deformed from a round billet to a rectangle one in the first pass, and then enters the second pass after rotating 90° around its axis. The main rolling conditions used and the information of billet are given in Table 1. Fig. 7 Workpiece deformation processes during firststep roll: (a) t=0.35 s; (b) t=0.5 s; (c) t=0.65 s; (d) t=0.8 s; (e) t=0.85 s; (f) t=0.9 s; (g) t=1.1 s; (h) t=1.3 s; Fig. 6 Finite element model of roll forging Table 1 Main parameters of rolling Parameter Value and description Billet material AISI 5140 Billet diameter/mm 140 Billet length/mm 855 Friction coefficient 0.5 −1 Rotational speed of roll/(rad∙s ) 1.8 Initial temperature of workpiece/°C 1100 Die temperature/°C 20 Environment temperament/°C 20 Heat transfer coefficient/ (N∙mm∙s −1 ∙°C −1 ) 11 Convection coefficient/ (N∙mm∙s −1 ∙°C −1 ) 0.02 Mesh number for billet 50000 3.2 Analysis of mechanism of defects In this section, the mechanism of defects during rolling forging process was analyzed, and complete attention has been paid on the reason why the size and shape of two spring boards are mismatched during firststep roll. Figure 7 shows the workpiece deformation process during firststep roll. By comparison, the FEM results basically accord with the observed results. Workpiece contour is the enveloping surface of rolling die and vice versa, while rolling die contour is the enveloping surface of forging piece [15]. From Figs. 7(a)−(c), when rolling the first spring board, the die is forced to bite into the workpiece, which brings thrust on workpiece along the x direction. So, the circumferential velocity of the roller surface is appr oximat el y equa l t o the a xial vel ocit y of th e workpiece at neutral plane, and the slip of workpiece along the die groove can be eliminated. For this reason, the dimension of first spring board can meet the design requirement after firststep roll. The deformation process of second spring board is shown in Figs. 7(d)−(g). The dimension of second spring board cannot meet the designed requirement, as shown in Fig. 7(h). There are two reasons for this phenomenon. Firstly, the crosssections of the grooves are rectangular at the second spring board and the rectangular groove only exerts a force on the top and bottom surface of workpiece, as shown in Fig. 4(a). So, the friction between die and workpiece is insufficient to make workpiece follow the movement of the die. Secondly, during the initial stage of rolling the second spring board, a thrust along the –x direction is imposed on workpiece by the die, and it can increase the relative sliding between workpiece and die. So, the relative motion between roll and workpiece is not consistent, as shown in Fig. 7(e). As discussed above, the bites condition and contact status of die and workpiece are different during rolling the first and second spring boards. To solve these problems, it is necessary to increase the die−workpiece contact area in the entry of deformation zone during the second spring board roll. 4 Die structure optimization In order to resolve the problems above, a new groove shape is presented as a substitute for the rectangular groove, and it is called ovaldiamond groove, as shown in Fig. (8). This groove has a slope on each of its two sides, and the top of the groove is a circular which is tangent to two slopes. As a combination of oval groove and diamond groove, the ovaldiamond groove puts pressure on the side of billet, and keeps space between die and workpiece on top and bottom. So, this J. Cent. South Univ. (2014) 21: 493−499 497 Fig. 8 Crosssection of ovaldiamond groove new groove can increase the contact area between die and workpiece, avoid the heterogeneous deformation, and increase the stability of billet at the same time. In order to test the effect of ovaldiamond groove, the deformation process of workpiece is analyzed by using FEM method. In this analysis, the parameters of groove are given as follows: R1=10 mm, R2=32 mm, R3=140 mm, β=90° and H=79.5 mm. Figure 9 shows the workpiece deformed by ovaldiamond groove roll. From Fig. 9, the size and shape of two spring board are almost the same. To analyze the difference between ovaldiamond and rectangular groove, the field variables in the cross section A of workpiece are discussed. Fig. 10 Effective stress contours of crosssection A at 0.45 s: (a) During rectangular groove rolling; (b) During ovaldiamond groove rolling Fig. 9 Workpiece after ovaldiamond groove roll (Unit: mm) 4.1 Stress field Stress is defined as the force acting on a unit area of material. The stress field of crosssection A at 0.45 s is shown in Fig. 10. It can be seen during ovaldiamond groove rolling and rectangular groove rolling, the effective stresses of workpiece are relatively high at contact area compared to other areas, and decrease with the reduction of distance from the contact area. From Fig. 10(a), for rectangular groove rolling, the minimum effective stress of section A is 49.5 MPa, and located at two sides, and the maximum effective stress is 72 MPa. From Fig. 10(b), for ovaldiamond groove rolling, the minimum value of 40.9 MPa occurs in the center of Section A, and the maximum value is 92 MPa. From above analysis, the effective stress of workpiece is relatively high under ovaldiamond groove rolling, which means that large friction can be obtained to improve the coordination of die rolling and the axial movement of the workpiece. 4.2 Strain field Strain is a measure of the deformation degree of an object. The strain distribution on crosssection A at 0.45 s is shown in Fig. 11. It can be observed from Fig. 11 that the maximum effective strain of workpiece occurs at the contact area, and decreases with the reduction of distance from the contact area. The maximum effective strain on Section A under ovaldiamond groove rolling is 0.235 and the minimum value of 0.0588 occurs in the center. The maximum strain value in rectangular groove is almost the same as that under ovaldiamond groove rolling. From above analysis, the deformation degree of workpiece is almost identical during two kinds of rolling, but larger effective stress can be obtained in the contact surface between the workpiece and the ovaldiamond groove. This means that the contact area between workpiece and die is expanded during ovaldiamond groove rolling. The forming load during ovaldiamond groove rolling is slightly larger than that during rectangular groove rolling, but less flow fluctuation can be obtained during ovaldiamond groove rolling, as shown in Fig. 12. 498 J. Cent. South Univ. (2014) 21: 493−499 Fig. 13 Roll dies in physical experiment Fig. 11 Effective strain contours of crosssection A at 0.45 s: (a) During rectangular groove rolling; (b) During ovaldiamond groove rolling roll forging machine. In order to save experiment funds, the experiment material is lead, which can be recovered and recycled. The workpieces at the end of each step are respectively shown in Fig. 14. Through measurement and comparison, the sizes of first and second spring board are almost the same, and all of them are in good agreement with design requirement. This groove can thoroughly eliminate the fold as well. Hence, less remanufacturing time and cost for automobile front axles are required. Furthermore, higher quality and lower cost products are generated. Fig. 14 Workpieces after two rolling pass: (a) First spring board; (b) Second spring board Fig. 12 Forming load during roll forging process 6 Conclusions 5 Physical experiment 1) The mechanism of mismatch during rollforging process is analyzed, and the main reason is the different bites condition and contact status between die and workpiece during rolling the first and second spring boards. 2) The ovaldiamond groove is presented as a substitute for rectangular one to reduce the defect. Ovaldiamond groove puts pressure on the side of billet, and keeps space between die and workpiece on top and bottom. It can increase the contact area between die and Based on above analysis, it can be concluded that ovaldiamond groove is in favor of improving forging quality. Subsequently, the physical experiment is carried out to test and validate the feasibility of this work. The workpiece is deformed from a round bar to an ovaldiamond one in the first step, and then enters into the hatshape groove after rotating 90° around its axis. Figure 13 shows the roll die installed on the DR461000 J. Cent. South Univ. (2014) 21: 493−499 workpiece, avoid the heterogeneous deformation, and increase the stability of billet. 3) Under the same condition of deformation degree, the large friction can be obtained on the contact surface between workpiece and the ovaldiamond groove. The forming load during ovaldiamond groove rolling is slightly larger than that during rectangular groove rolling, but the less flow fluctuation can be obtained during ovaldiamond groove rolling. 4) The physical experiment validates that the ovaldiamond groove can resolve defect perfectly, and the size of part is in good agreement with design requirement. 499 [6] [7] [8] [9] [10] References [1] [2] [3] [4] [5] HU Zhenghuan, ZHANG Kangshen, WANG Baoyu, SHU Xuedao, YANG Cuiping. 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