Wear 244 (2000) 41–51 Effects of lubrication and die radius on the friction behavior of Pb-coated sheet steels Zhi Deng, M.R. Lovell∗ Department of Mechanical Engineering, University of Pittsburgh, Pittsburgh, PA 15261, USA Received 11 January 2000; received in revised form 19 April 2000; accepted 19 May 2000 Abstract Using a strip tensile friction simulator, the influence of lubricant properties (viscosity and extreme pressure) and pin radius on the interfacial friction and the surface quality of Pb-coated sheet steels is investigated. Nine distinct testing conditions are examined by varying the lubricants (three oils and two greases) and pin radii (10 and 20 mm). Friction coefficient curves are generated as a function of sliding distance for each condition examined and the surface quality of the sheets are evaluated from surface roughness and micrographs taken before and after testing. From the experimental results, tendencies for the interfacial friction and surface finish of Pb-coated sheet steels are established with respect to lubricant properties and pin radius. Specifically, the results indicated that the friction coefficient increases with both the viscosity and extreme pressure (oils only) of the lubricants. In addition, it was determined that the lubricant properties had little influence on the final surface roughness of the deformed sheet. Considering the influence of pin size, the results showed that the friction coefficient increased with decreasing pin radius values. © 2000 Elsevier Science S.A. All rights reserved. Keywords: Lubrication; Pb-coated sheet; Friction 1. Introduction Due to their anti-corrosive properties, Pb-coated sheet steels have been prevalently used throughout the automotive industry in the manufacturing of oil pans and fuel tanks. Despite the recent introduction of plastics and other specialized coatings, Pb-coated sheets are still the primary material used in anti-corrosion automotive applications, particularly in eastern Europe and Asia. One common characteristic of the parts produced using Pb-coated sheets is that their geometries are fairly complex in nature. This makes the formation of Pb-coated parts difficult, as most geometries must be produced under lubrication using a single or multiple stage deep-drawing process. Due to the large strain deformations that develop during deep-drawing, failure within the sheet commonly occurs in areas of high strain. As shown in Fig. 1, the primary failure mechanisms within the sheet are characterized by (1) wrinkling along the flange and die lip regions, and (2) wall fracture along the punch lip region. Both of these failures are directly dependent on the interfacial friction that develops between ∗ Corresponding author. Present address: Department of Mechanical Engineering, University of Pittsburgh, Pittsburgh, PA 15261, USA. Tel.: +1-412-624-9601; fax: +1-412-624-4846. E-mail address: [email protected] (M.R. Lovell). the forming tools and the sheet, especially in the punch and die lip regions [1]. In order to reduce friction and minimize sheet failure, lubricants are typically applied to portions of the workpiece that undergo severe contact with dies. In fact, lubrication is still the most economical and effective method for reducing the harmful effects of large interfacial friction forces that can develop in stamping operations. During the stamping of automobile components, the type of applied lubricant is a critical parameter in determining the overall quality of the final part. When lubricants, such as oils and greases are applied to the workpiece, the frictional resistance of the sheet material decreases and the strain uniformity of the sheet increases. This ultimately improves the overall formability and surface quality of the workpiece. Due to differences in material properties and deformation behavior, however, the effect of lubrication distinctly varies with sheet metal coating material. In particular, Pb-coated sheet steels are known to deform much differently than Zn-coated sheet steels under identical stamping conditions. This is particularly important when one considers that almost all of the published frictional studies of stamping operations have investigated galvanized sheet steels [2–7]. For this reason, it is essential to characterize the nature of interfacial friction in stamping processes that utilize Pb-coated sheet steels. By conducting the frictional investigations for both galvanized and Pb-coated sheet steels under identical conditions, the 0043-1648/00/$ – see front matter © 2000 Elsevier Science S.A. All rights reserved. PII: S 0 0 4 3 - 1 6 4 8 ( 0 0 ) 0 0 4 3 0 - 0 42 Z. Deng, M.R. Lovell / Wear 244 (2000) 41–51 Fig. 1. Failures in the workpiece during deep-drawing process. difference in lubrication between Zn- and Pb-coated sheet steels can be ascertained [8]. Since lubricants are currently being selected using trial and error techniques, developing correlations between lubricant properties, interfacial friction and surface finish quality of Pb-coated sheet steels would greatly benefit designers and automobile manufactures. With such information, the effects of lubricant on the friction and formability of terne-coated sheet steels could be more accurately predicted and controlled. 2. Methods of testing 2.1. Tensile strip friction tests Previous investigations on sheet metals [9,10] have found that frictional forces in stamping processes are a complicated function of material properties, process parameters and contacting conditions so that it is difficult to construct a single experimental test that fully represents the frictional behavior of a sheet metal forming process. Therefore, in order to assess the interfacial friction properly, it is necessary to carry out experiments under conditions that closely represent an actual production process. In forming complex parts, such as automotive oil pans, many convex–concave shapes (lips) are subject to a complicated stress state that includes tension, compression, bending and shear. These shapes have large strains and often develop faults during the forming process. As a result, lips typically become an emphasis in the design and optimization of automotive forming processes [1]. For this reason, a strip tensile friction simulator (see Fig. 2) was utilized in the current investigation. Similar to that developed by Duncan et al. [11], the apparatus used was a ‘plane-strain bend/unbend tension’ device that stretches and bends sheet metal strip specimens during testing so that the frictional effects can be simulated near the lip regions of Fig. 2. Tensile strip friction testing apparatus. a forming process. By means of the testing apparatus, the friction coefficient between the die and the workpiece, as well as the surface roughness of the deformed sheets, could be measured over a wide range of operating conditions. It is important to note that such an apparatus does not exactly capture the conditions of a classical deep drawing process where high compressive stresses and strains develop in the lips. Friction tests were carried out on sheet metal strips using a MTS 318.10-type material tensile testing machine that was modified to include a specially designed friction measurement system. Fig. 2 shows a schematic view of the friction measurement system and its overall dimensions. As depicted, the system was rigidly attached to the loading and clamping heads of a tensile testing machine. Prior to each test, a strip specimen was bent around the two pins to simulate the lip region of the dies in a sheet metal forming process. Both ends of the strip specimen were tightly held by two catchers. Then, loading of the tensile machine produced significant plastic deformation in the strip. As the load was increased, the plastic deformation in the strip continuously increased until a neck or a crack developed at some point along the vertical portions of the strip. During the loading process, two extensometers that are mounted on the vertical and horizontal portions of the strip continuously measure extensions E1 and E2 as shown in Fig. 2. The forming load, 2P1 , is simultaneously recorded from the tensile machine so that load-extension curves similar to that depicted in Fig. 3 can be produced. Since the metal strip consists of a uniform material, the recorded load versus strain curves are valid for all portions of the strip. For this reason, the force P2 can be accurately estimated and the friction coefficient between the specimen and pins, µ, as well as the sliding distance, S, Z. Deng, M.R. Lovell / Wear 244 (2000) 41–51 43 Fig. 3. The experimental tensile force-extension curves. along the pin can be determined for each condition tested. The procedure for determining µ and S is outlined in the following section. The forces acting on the portion of a sheet strip contacting the pin are illustrated in Fig. 4. Assuming that there is a constant friction coefficient in the contact region, µ, consider a section of the strip along the wrap angle, θ , at some instant during deformation. From Fig. 4, and according to the equilibrium of all the forces acting on an elemental cut of the strip, dθ, it can be shown that: P + µqwR dθ − (P + dP ) = 0 dθ =0 qwR dθ − (P + dP + P )sin 2 (1) (2) where q is unit normal pressure and w the width of the strip. We will assume that dθ is very small so that dθ dθ ≈ (3) sin 2 2 Fig. 4. Forces acting on an elemental cut of the strip. and dP P (4) Combining Eqs. (1)–(4) we find dP = µ dθ P (5) Integrating Eq. (5), friction coefficient µ is determined to be P1 2 (6) µ = ln π P2 The overall sliding distance of the strip over one of the pins can be calculated by the following equation due to the symmetry of the apparatus: S = (a − R)E1 (7) The extension of the sheet, E1, is an important parameter because it not only determines the amount of sliding of the sheet over the pins but also represents the deforming limit of a specimen. By recording the value of E1 during the test until the specimen cracks, the formability of the deformed sheets can be ascertained under specific lubrication conditions. It is important to note that in the apparatus, only the sliding bend and unbend effects are captured in the plastic deformation of the strip specimen. It is clear from the testing procedure that the measured loading force, 2P1, and tangential force, P2, include the forces that develop as the sheet bends around the pins. The calculated friction coefficient (Eq. (6)), however, does not explicitly include a bending force term. Similar to the apparatus used by Hao et al. [12], the actual bending force cannot be uncoupled and used in the calculation of the friction coefficient. In other types of testing systems, such as that introduced by Wilson et al. [13], the bending force can be directly measured by 44 Z. Deng, M.R. Lovell / Wear 244 (2000) 41–51 replacing the pins by rollers. For this case, the bending force, Pb , has been shown to be: Table 2 Physical properties of lubricants Items σy t 2 w , Pb = 2r (8) where t is the thickness of the sheet, w the width of the sheet, and r the radius of the pin. Then, using Eq. (8), expressions for the friction coefficient can be generated that include the bending force directly. 2.2. Testing conditions By means of the testing apparatus, the interfacial friction coefficient between the die and the sheet could be measured over a wide range of operating conditions by varying lubricant and die profile radius. In the tests conducted, the speed of the tensile testing machine was fixed at 25.4 mm/min. The gauge lengths of both extensometers E1 and E2 were 50 mm. The pin radii, R, used in the investigations were 10 and 20 mm, respectively. Both pins consisted of 45# mild carbon steel and had a surface hardness of HB=240 and an initial surface roughness, Ra , of 0.15 m. Five different lubricants, three oils and two greases were applied to the sheet steel. A total of nine distinct testing conditions were examined by varying pin radius and lubricant. 2.3. Sheet material composition and lubricant properties The chemical composition and mechanical properties of the Pb-coated sheet steel analyzed in the experiments are listed in Table 1. In Table 1 YS, TS, EL and IE are respectively, the yield stress, tensile strength, total elongation and Erichsen value of the studied material. For the material examined, specimens were cut from the sheet as parallel-sided strips that were 500.0 mm long, 20.0 mm wide and 1.0 mm thick. Both parallel sides of each specimen were carefully polished and maintained a parallel error of <0.013 mm. It has been determined that the most important indices among lubricant properties related to sheet metal forming are density, viscosity and extreme pressure [8]. The extreme pressure is defined as the maximum contact pressure the lubricant film can withstand without allowing significant asperity contact to occur between surfaces. In order to examine the effect of lubricant, three commercial oils and two commercial greases were selected. The density, viscosity and extreme pressure of these lubricants were respectively, measured by means of an optoelectronic balance, an automatic kinematic viscometer and a 4-ball EP tester using standard Oil #1 Oil #2 Oil #3 Grease #1 Grease #2 20◦ C, Density (at g/ml) 0.85 0.87 0.93 1.01 1.12 Viscosity (at 40◦ C, Pa s) 0.046 0.277 0.074 0.740 1.330 Extreme pressure (N) 1078.0 441.0 981.0 <98.0 <98.0 Table 3 The measured surface roughness of the studied Pb-coated sheet steel tested under different conditions The initial surface roughness Lubricant Ra (m) Rm (m) The surface roughness after deformation R=20 mm Ra (m) 0.40 1.03 Dry 0.50 Oil #1 0.67 Oil #2 0.65 Oil #3 0.65 Grease #1 0.67 Grease #2 0.68 R=10 mm Rm (m) Ra (m) Rm (m) 3.32 5.47 7.25 4.70 4.55 5.53 NA 0.40 0.55 NA NA 0.53 NA 3.58 7.10 NA NA 3.80 testing methods. The average density, viscosity and extreme pressure for each lubricant are listed in Table 2. Prior to testing, the pins and the strip specimen were cleaned with acetone and uniformly lubricated or kept dry to measure the friction coefficient. After each test, the pins were polished with fine emery cloth (600 grit) to remove possible lead build-up. 2.4. Surface roughness measurement and microscopic surface observation The surface roughness values of the original and deformed Pb-coated sheet specimens were obtained using a VIDEO T20-type 3-D automatic profilometer. The mean, Ra , and maximum, Rm , surface roughness, within each examined segment were measured for three to five times on the surface which made contact with the pins, along the directions, respectively, parallel and perpendicular to the sliding direction of the specimen in the frictional test. The final measured surface roughness values are the averages of these measurements and listed in Table 3 for the lubricants and pin radii tested. For the purpose of evaluating the influence of lubricant properties and pin radius on the surface quality of the Table 1 Chemical composition and mechanical properties of the studied material Material Pb-coated sheet steel Chemical composition (wt.%) Mechanical properties Coating thickness (m) C Si Mn P S Al YS (MPa) TS (MPa) EL (%) IE (mm) 0.0076 ≤0.05 0.16 0.012 0.004 – 161.5 303.9 46.6 11.4 5.71/4.95 Z. Deng, M.R. Lovell / Wear 244 (2000) 41–51 deformed sheets, the surfaces of the sheets were observed and photographed before and after testing using an optical microscope. The samples evaluated were obtained by cutting portions of the deformed sheets that directly contacted the pins. Prior to observation, the deformed sheet specimens were straightened and cleaned using acetone. It is important to note that both the surface roughness measurements and the microscopic surface observations are imperative for understanding the relationship between the surface quality and the interfacial friction during the stamping of terne-coated sheet steels. 45 thickness equations can be used to determine the conditions required for two surfaces to operate in the EHL regime [17]. It is important to note, however, that Hamrock and Dowson’s equations will only provide a relative estimate of the conditions required for EHL in our apparatus. This is due to the fact that the central film thickness expressions were derived for a spherical contact condition, whereas the contact in our apparatus is more cylindrical in nature. From Hamrock and Dowson’s work, the following expression can be used to predict the critical velocity at which two surfaces will be entirely separated by a film of lubricant: G−0.791 W 0.1 V = 0.228E 0 RH1.493 C ×(1 − 0.61e−0.73 )−1.493 η−1 3. Discussion of results 3.1. Effect of lubricant Before discussing the results of the tensile frictional tests, it is important that a brief description is given on the nature of lubrication in large strain stamping processes. Prior work [13] has found that the contact pressure between the sheet and the die in stamping is relative low so that the frictional interaction between surfaces is carried out through mixed lubrication asperity contact that is dominated by boundary effects. Under such conditions, the total applied load is partially carried by the hydrodynamic action of the lubricant film as well as the predominant asperity contacts. The total friction force is then a combination of viscous friction and asperity interaction [14]. In stamping, sliding asperity contact between the die and workpiece surfaces can cause both abrasion and adhesion. Naturally, viscosity and extreme pressure of the applied lubricants will play an important role in defining the nature of the asperity interaction. Specifically, a lubricant with high viscosity can form a thicker film, enlarging the distance between the interacting asperities and reducing their abrasion. Furthermore, a lubricant with high extreme pressure may keep an oil film under higher contact pressure between two asperities and minimize the possibility of asperity adhesion [14,15]. Therefore, the tribological interaction between contacting surfaces in sheet metal stamping must be considered a complex function of the properties of the applied lubricants. As demonstrated by the fundamental Stribeck curve, the magnitude of friction between two surfaces dramatically changes with lubrication regime. In boundary lubrication (BL), for example, the friction coefficient is relatively high because there is considerable asperity interaction between the contacting surfaces. In elastohydrodynamic lubrication (EHL), on the other hand, the friction coefficient is significantly lower than BL because a film of lubricant entirely separates the asperities of the surfaces in contact. To gain insight into the physical nature of friction between the pin and sheets, it is important to establish the lubrication regime for which our experiments were conducted. This can be accomplished utilizing the central film thickness equations developed by Hamrock and Dowson [16]. The central film where " (1 − ν12 ) (1 − ν22 ) + E0 = 2 E1 E2 (9) #−1 (10) H0 R (11) G= E0 piv,as (12) W = F E0R (13) HC = In the preceding equations, E0 is the effective elastic modulus, E1 , E2 , ν 1 and ν 2 are the respective elastic moduli and Poisson’s ratios of the sheet and pins, HC the minimum film thickness parameter, H0 the film thickness of the lubricant, R the pin radius, G the dimensionless material parameter, F the total force acting on the sheet from each pin, piv,as the asymptotic isoviscous pressure, and W the dimensionless load parameter. Table 4 lists several of the material parameters in our experimental system. Using the values in Table 4, Eq. (9) can be used to predict the critical sliding speed for which EHL develops in our apparatus once F and H0 are determined at a given operating condition. To determine the critical velocity, the force F can be established using the work of Hao et al. [12]. In Hao’s work, detailed discussion was given for the pin/strip contact conditions found in the current work. For the geometry shown in Fig. 5, Hao introduced the following governing (Reynolds’) equation for the pressure distribution: Pi = Pi−1 + x 2 (xi − xi−1 ) 3ηV × i−1 2 R (H0 + (xi−1 /2R)) (14) Table 4 The related material parameters for determining the critical speed Sheet elastic modulus (E1 ) Pin elastic modulus (E2 ) Sheet Poisson’s ratio (ν 1 ) Pin Poisson’s ratio (ν 2 ) Asymptotic isoviscous pressure (piv,as ) 81.0 GPa 207.0 GPa 0.28 0.30 4.795×107 Pa 46 Z. Deng, M.R. Lovell / Wear 244 (2000) 41–51 Fig. 5. Geometry of the interface between the sheet and pin. where P is the pressure of the fluid, H0 the film thickness at x=0, V the sliding speed of the strip, and η the lubricant viscosity. Assuming that the film thickness of the lubricant (H0 ) is equivalent to the combined effective surface roughness of the Pb-coated sheets and pins (0.427 m), the pressure distributions can be determined for different lubricants and pin radii using the parameters given in Tables 2 and 3. Once the pressure distribution is known, the force F can be determined by multiplying the average contact pressure by the known contact area between the pin and sheet. As an example, consider the case of oil #2 at a pin radius of 20 mm. For this case, the maximum pressure produced between the pin and sheet will be 0.1407 Pa and the critical speed for EHL to develop is 44.39 mm/s. Comparing this velocity to the velocity used during our experiments (0.423 mm/s), it is very likely that our experiments were dominated by boundary lubrication effects. It is important to note that the determination of the critical velocity in this section was an idealized solution to a complicated phenomenon, and was merely intended to provide a relative comparison of lubrication in the current investigation. 3.1.1. Grease lubricants Examining Table 2 we find that the grease #1 and #2 have distinctly different viscosities, while their density and extreme pressures are nearly identical. Hence, by plotting the experimentally measured friction coefficient as a function of the sliding distance for both greases (as shown in Fig. 6), several trends for the effect of grease lubricant viscosity on the friction characteristics of the Pb-coated sheet steels can be ascertained. The first trend shows that when compared to the dry condition, both greases reduce the interfacial friction coefficient by more than a factor of two. Such a tendency is in good agreement with boundary lubrication theory where the addition of a lubricant will decrease abrasive asperity interaction between the sheet and the dies as the lubricant ‘fills’ the valleys of the contacting surfaces. A second notable trend in Fig. 6 is that the friction coefficient for grease #2 is greater than that of grease #1 over the entire range of sliding distance. This trend can be explained by the fact Fig. 6. Comparison of lubricating effect of both grease lubricants for a pin radius of 20 mm (grease #1 and #2). that the grease #2 has a significantly higher viscosity than the grease #1. Since the contact between the sheet and die is dominated by boundary effects, the higher viscosity lubricant will have a larger internal shear resistance as the die and sheet surfaces slide relative to one another and ‘push’ the lubricant through the pin-sheet interface. A final tendency found in Fig. 6 is that the friction coefficient of both greases remains essentially constant with respect to sliding distance. This is to be expected because at the speeds tested, the boundary lubrication effects of the grease will remain uniform when sufficient amounts are applied to the contacting surfaces. 3.1.2. Oil lubricants Unlike the grease lubricants that only vary in viscosity, Table 2 shows that the three oils evaluated distinctly vary in both viscosity and extreme pressure. Then, by plotting the measured friction coefficient versus the sliding distance for the three oils, we can determine the combined influence of lubricant viscosity and extreme pressure on the friction characteristics of the Pb-coated sheet steels. Fig. 7 depicts the measured friction coefficient for the three oils evaluated at a pin radius of 20 mm. Comparing the curves for Fig. 7. Friction coefficient curves of the Pb-coated sheet steel for three oils and a pin radius of 20 mm. Z. Deng, M.R. Lovell / Wear 244 (2000) 41–51 all three oils in the figure, we observe that oil #2 has the lowest friction coefficient while oil #1 has the highest one. Considering the properties of each lubricant in Table 2, we find that the friction coefficient increases with lower oil viscosity and with higher oil extreme pressure. Combined with the relative variation of friction coefficient with grease viscosity and extreme pressure, it is deduced that the extreme pressure plays a more significant role than viscosity in determining the overall friction coefficient of Pb-coated sheet steels. As discussed above, when lubricant extreme pressure is lower as in the grease, the interaction between the sheet and die is characterized by a boundary lubrication regime where the interfacial friction coefficient increases with increasing lubricant viscosity. When lubricant extreme pressure is high enough such that the oil film on the interface is maintained during the entire contact process, the interaction between the sheet and die will be dominated by a mixed lubrication regime. Sometimes referred to as partial lubrication, a mixed lubrication regime exhibits both boundary and fluid-film effects. In this regime, more viscosity oils will fill and be trapped in the cavities between the asperities to a great extent in comparison to less viscosity oils. This ‘filling’ increases the fluid pressure generated within the cavities, causing a more substantial ‘separation’. As a result, the interfacial friction coefficient becomes lower. Therefore, the 47 influence of lubricant viscosity on the interfacial friction behavior in a Pb-coated sheet steel stamping operation should be evaluated together with lubricant extreme pressure. 3.1.3. Surface roughness and surface quality Table 3 lists the mean, Ra , and maximum, Rm , surface roughness values of the Pb-coated sheet steels before and after the friction tests were performed. As shown in the table, the mean surface roughness of the Pb-coated sheets increased by more than 60% after testing for each of the lubricants examined. This increase of surface roughness occurs from the abrasive interfacial asperity interaction that occurs when the coated sheets slide and plastically deform over the pin. Comparing the mean surface roughness, Ra , of different lubricants after testing, one finds that lubricant viscosity and extreme pressure appear to have little effect on the average surface roughness. In fact, for each of the five lubricants tested at R=20 mm, the mean surface roughness variation was between 0.65 and 0.68 mm. Such a small difference in roughness is insignificant compared to the variation in lubricant viscosity and extreme pressure which show larger maximum differences in extreme pressure (98.0–1078.0 N) and viscosity (0.046–1.330 Pa s). In order to further evaluate the effect of lubricant properties on the surface quality of the deformed sheets, Figs. 8 Fig. 8. The surface micrographs of the deformed Pb-coated sheet steel for both greases and a pin radius of 20 mm. 48 Z. Deng, M.R. Lovell / Wear 244 (2000) 41–51 Fig. 9. The surface micrographs of the deformed Pb-coated sheet steel for three oils and a pin radius of 20 mm. and 9 were created. Fig. 8 depicts micrographs of the undeformed and deformed sheet surfaces for the two greases analyzed, and Fig. 9 consists of micrographs of the deformed sheets for the three oils examined. From Figs. 8 and 9 several trends can be ascertained for the role of lubricant properties on the overall surface quality of Pb-coated sheet steels. The first notable trend is that all of the deformed sheet surfaces in Figs. 8 and 9 have significantly different surface finishes from the initial coated sheet surface depicted in Fig. 8(a). In Fig. 8(a), it is found that the undeformed coated sheet has a relatively smooth surface finish with a minor peaks and valleys and no distinguishable markings. In each of the deformed specimens of Figs. 8 and 9, however, one finds that the distinctive tracks or craters developed on the Pb-coated sheet during the friction tests. Another notable trend in Fig. 8 is that the viscosity of the grease lubricants has a significant impact on the overall surface finish of the deformed sheets. In the micrograph for the lower viscosity grease #1 of Fig. 8(b), there is more severe roughening of the coating surface than in the micrograph for the higher viscosity grease #2 of Fig. 8(c). In fact, the overall surface wear patterns are distinctly different for the two greases analyzed. For the low viscosity grease, there are pronounced uniform sliding tracks along the Pb-coated sheet surface. These sliding tracks indicate that significant asperity abrasion occurred along the entire contact region between the pin and sheet during sliding. For the high viscosity grease, however, there are no obvious sliding tracks but a series of micro-craters on the deformed sheet surface. Such a wear pattern would indicate that only localized asperity abrasion took place between the pin and Pb-coated sheet. As discussed previously, the higher viscosity lubricants are better for reducing the abrasion along the contact interface. Despite these benefits, the highest viscosity lubricants may not be able to eliminate localized abrasion at between the highest asperity peaks. The formation of the micro-craters on the sheet surfaces would indicate that grease #2 did not fully separate the pin and sheet surfaces during the sliding tests. A final tendency of the dependence of surface finish on lubricant properties can be deduced by examining the oil lubricant micrographs of Fig. 9. In the micrographs for the three oils tested, the lower friction coefficient lubricants, oil #2 and oil #3, show more pronounced wear tracks than the oil #1. This fact occurred although the final surface roughness values of the steels tested with the three lubricants are virtually the same. This can be explained by the fact that a higher extreme pressure lubricant will minimize asperity interaction by carrying a larger amount of the load during mixed lubrication. Then, as the coated sheet Z. Deng, M.R. Lovell / Wear 244 (2000) 41–51 steel slides relative to the pin, less abrasion will occur between the surfaces, thereby reducing the depth of the wear tracks that develop. Because Pb-coated sheet steels are not typically utilized in surface critical applications, however, the frictional properties of the applied lubricant should be considered the most important parameter when selecting a lubricant in Pb-coated sheet steel applications. 3.2. Effect of pin radius 3.2.1. Friction coefficient Along with determining the influence of lubricant properties, a second variable investigated during the friction tests was the pin radius. In particular, tensile strip tests were performed on the Pb-coated sheet steels at pin radii of 10 and 20 mm. Since the strip testing system was designed to highlight the strain characteristics of the die lip region in a stamping process, the smaller radius pins (10 mm) represent a stamping operation with a sharper lip. It is typically difficult to design forming dies when stamping sharp lips because failure often occurs (see Fig. 1) as the coated sheet undergoes large strains. In order to establish the character of the friction while varying the pin radius, Fig. 10 was generated. Fig. 10 plots the measured friction coefficient as a function of the sliding distance for oil #1, oil #2, and grease #2 at both pin radii. As shown in the figure, we find that for all three lubricants, the friction coefficient increases at the smaller pin radius. This is to be expected because the plastic bending effect in the material region contacting the pins increases for smaller pin radius. The increased bending force causes the inside material to have stronger compressive stress, which further increase the interaction between the contacting asperities. Such an increased asperity interaction will then increase the overall friction coefficient between the sheet and the pins, as demonstrated at the smaller pin radius (10 mm) in Fig. 10, because more energy is dissipated for this additional component. Hence, it can be deduced that the friction coefficient between the Fig. 10. Influence of pin radius on the friction behavior of the Pb-coated sheet steel for different lubrications (oil #1 and #2, grease #2). 49 forming dies and Pb-coated steel sheets will increase as sharper lips are formed in a stamping operation. Although there was minimal build-up of the lead coating on the pins during most of the friction experiments, it is important to note that there were two specific operating conditions where substantial lead residue was found. The first condition that produced build-up was for oil #1 at R=10 mm. The lead residue in this case can be attributed to the combined effects of the low viscosity of oil #1 and the small contact area of the 10 mm pin. Under these conditions, the interfacial abrasion between the sheet and pins was significantly more severe than the other lubricated cases, which caused more of the softer lead material to be deposited onto asperities of the pins. In fact, as indicated in Fig. 10, the lead build-up at this condition caused unique behavior in the friction coefficient curve. In the figure, the friction coefficient initially increased during sliding before a maximum value was attained. After reaching this maximum value, µ decreased in a manner identical to the other lubricants in Fig. 10. One explanation for this phenomenon is that as the sheet progressed along the pin, the amount of coating material on the pins gradually accumulated until a critical level was reached where most of the pin/sheet asperities were separated. Once attaining this critical coating level, the abrasion between the sheet and pin became constant or decreased, as indicated by the lower friction coefficient values at greater sliding distances. A similar tendency was also observed for the dry condition, where the high level of abrasion also resulted in a significant Pb residue on the pins. As shown in Fig. 6, however, the build-up does not appear to attain a critical level as with oil #1. For the dry case, the friction coefficient increased throughout the testing after an initial ‘sticking period’ is overcome. This sticking period occurs because there is initially significant adhesion in the absence of lubricant and the sheet must actually ‘break away’ from the pins at the onset of motion. The later increase in friction coefficient would indicate that significant separation between the pin/sheet asperities does not occur in the absence of a lubricant and that the lead continued to build-up on the pins over the entire sliding distance. Using the two specific conditions as a basis, it would appear that higher viscosity lubricants would be beneficial for eliminating build-up when stamping Pb-coated sheet steels, especially when a die with a sharp lip is utilized. 3.2.2. Surface roughness and surface quality In addition to quantifying the friction coefficient, determining the influence of pin radius on the overall surface quality of the deformed sheet is also extremely important in stamping processes. For this purpose, Fig. 11 was created to show the final surface finish at the two pin radii tested. Initially examining Table 3, we find that the average surface roughness of the deformed sheets is lower for a pin radius of 10 mm than for a pin radius of 20 mm. In addition to a smaller surface roughness, Fig. 11 also demonstrates that the smaller radius pin produced a smoother surface than 50 Z. Deng, M.R. Lovell / Wear 244 (2000) 41–51 Fig. 11. Comparison between the surface micrographs of the deformed Pb-coated sheet steel for different pin radii and lubricants. the larger radius pin for oil #1 and oil #2. In particular, the larger radius deformed sheets have more pronounced wear tracks than the smaller radius sheets. It is important to note that an identical result was found in Figs. 8 and 9 where the smoothest surface finish was obtained under the conditions that yielded the highest friction coefficient. This phenomenon can best be explained by considering the physical interaction between the sheet and the pins at a higher surface pressure. At a smaller pin radius, higher contact pressures develop, which leads to more substantial plastic flow of both the Pb-coated sheet and pin asperities acting along contact interface. This increase in plastic flow along the interface is marked by an increase in adhesion, rather than abrasion, as shown in the micrographs of Fig. 11. The adhesive interaction between asperities causes a smoother surface finish with micro-craters while abrasion is characterized by sliding wear tracks. Hence, despite having an increased friction coefficient, a sharp lip in a stamping process may yield smoother surface finishes than a rounded lip. 4. Summary and conclusions In this work the frictional characteristics of Pb-coated sheet steels have been investigated using a tensile strip test- ing system. From the experimental results, the following conclusions were obtained: 1. For the grease lubricants analyzed, the friction coefficient between the sheet and dies was found to increase with increasing lubricant viscosity. 2. For the oil lubricants analyzed, the friction coefficient increased with increasing lubricant extreme pressure and with decreasing lubricant viscosity. In addition, the extreme pressure of the oil was found to play a more substantial role than the oil viscosity in determining the overall friction coefficient. 3. The lubricant properties were found to have little influence on the final surface roughness of the deformed sheets. 4. When considering surface quality, lubricant properties were found to play a critical role. In particular, a smoother surface finish was attained for lubricants with higher viscosity and extreme pressures values that produced a larger friction coefficient. 5. At a smaller pin radius, which corresponds to the stamping of a sharper lip, the friction coefficient between the contacting sheet and pin surfaces increased and the final surface roughness of the deformed sheets decreased. Smaller pin radius was also found to be liable to the occurrence of lead build-up. Z. Deng, M.R. Lovell / Wear 244 (2000) 41–51 Since very little work has been performed on determining the tribological behavior of Pb-coated sheet steels, the above results represent an important step in helping manufacturers effectively to select lubricants for large strain stamping processes. 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Part III. Fully flooded results, ASME J. Lubrication Technol. 99 (1977) 264–276. [17] M.R. Lovell, M.M. Khonsari, R.D. Marangoni, The response of balls undergoing oscillatory motion: crossing from boundary to mixed lubrication regimes, ASME J. Tribol. 115 (1993) 261– 266. 本文献由“学霸图书馆-文献云下载”收集自网络,仅供学习交流使用。 学霸图书馆(www.xuebalib.com)是一个“整合众多图书馆数据库资源, 提供一站式文献检索和下载服务”的24 小时在线不限IP 图书馆。 图书馆致力于便利、促进学习与科研,提供最强文献下载服务。 图书馆导航: 图书馆首页 文献云下载 图书馆入口 外文数据库大全 疑难文献辅助工具
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