APPARATUS FOR ELECTRICAL-ASSISTED INCREMENTAL FORMING AND PROCESS THEREOF

FIELD OF THE INVENTION

The present invention is related to the deformation of metallic materials, and more particularly, related to the deformation of metallic materials while passing an electric current therethrough.

BACKGROUND OF THE INVENTION

During forming of metals using various bulk and sheet deformation processes, the required magnitude of force to perform deformation is a significant factor in terms of the manufacturing of parts. For example, as the required force for deformation increases, larger equipment must be utilized, stronger tools and dies are required, tool and die wear increase, and/or more energy is consumed in the process. Furthermore, all of these factors increase the manufacturing cost of a given component and a process or apparatus that would decrease the required force for deformation and/or increase the amount of deformation that can be achieved without fracture and/or retain the deformed shape after unloading could have a significant impact on many manufacturing processes.

Presently, deformation forces are reduced, elongations are increased and deformed shapes are maintained by working metals at elevated temperatures. However, significant drawbacks to deforming materials at elevated temperatures exist, such as increased tool and die adhesion, decreased die strength, decreased lubricant effectiveness, decreased dimensional accuracy and consumption of materials for heating (which raises energy cost), and the need for additional equipment to be purchased.

One possible process of deforming metallic materials without using such elevated temperatures is to apply an electric current to the workpiece during deformation. In 1969, Troitskii found that electric current pulses reduce the flow stress in metal (Troitskii, O. A., 1969, zhurnal eksperimental'noi teoreticheskoi kiziki/akademi'i'a nauk sssr—pis'ma v zhurnal .eksperimental' i teoretiheskoi fiziki, 10, pp. 18). In addition, work by Xu et al. (1988) has shown that continuous current flow can increase the recrystallization rate and grain size in certain materials (Xu, Z. S., Z. H. Lai, Y. X. Chen, 1988, “Effect of Electric Current on the Recrystallization Behavior of Cold Worked Alpha-Ti”, ScriptaMetallurgica, 22, pp. 187-190). Similarly, works by Chen et al. (1998, 1999) have linked electrical flow to the formation and growth of intermetallic compounds (Chen, S. W., C. M. Chen, W. C. Liu, Journal Electron Materials, 27, 1998, pp. 1193; Chen, S. W., C. M. Chen, W. C. Liu, Journal Electron Materials, 28, 1999, pp. 902).

Using pulses of electrical current instead of continuous flow, Conrad reported in several publications that very short-duration high-density electrical pulses affect the plasticity and phase transformations of metals and ceramics (Conrad, H., 2000, “Electroplasticity in Metals and Ceramics”, Mat. Sci. & Engr., A287, pp. 276-287; Conrad, H., 2000, “Effects of Electric Current on Solid State Phase Transformations in Metals”, Mat. Sci. & Engr. A287, pp. 227-237; Conrad, H., 2002, “Thermally Activated Plastic Flow of Metals and Ceramics with an Electric Field or Current”, Mat. Sci. & Engr. A322, pp. 100-107). More recently, Andrawes et al. has shown that high levels of DC current flow can significantly alter the stress-strain behavior of 6061 aluminum (Andrawes, J. S., Kronenberger, T. J., Roth, J. T., and Warley, R. L., “Effects of DC current on the mechanical behavior of AlMg1SiCu,” A Taylor & Francis Journal: Materials and Manufacturing Processes, Vol. 22, No. 1, pp. 91-101, 2007). Complementing this work, Heigel et al. reports the effects of DC current flow on 6061 aluminum at a microstructural level and showed that the electrical effects could not be explained by microstructure changes alone (Heigel, J. C., Andrawes, J. S., Roth, J. T., Hoque, M. E., and Ford, R. M., “Viability of electrically treating 6061 T6511 aluminum for use in manufacturing processes,” Trans of N Amer Mfg Research Inst, NAMRI/SME, V33, pp. 145-152).

The effects of DC current on the tensile mechanical properties of a variety of metals have been investigated by Ross et al. and Perkins et al. (Ross, C. D., Irvin, D. B., and Roth, J. T., “Manufacturing aspects relating to the effects of DC current on the tensile properties of metals,” Transactions of the American Society of Mechanical Engineers, Journal of Engineering Materials and Technology, Vol. 29, pp. 342-347, 2007; Perkins, T. A., Kronenberger, T. J., and Roth, J. T., “Metallic forging using electrical flow as an alternative to warm/hot working,” Transactions of the American Society of Mechanical Engineers, Journal of Manufacturing Science and Engineering, vol. 129, issue 1, pp. 84-94, 2007). The work by Perkins et al. (2007) investigated the effects of currents on metals undergoing an upsetting process. Both of these previous studies included initial investigations concerning the effect of an applied electrical current on the mechanical behavior of numerous materials including alloys of copper, aluminum, iron and titanium. These publications have provided a strong indication that an electrical current, applied during deformation, lowers the force and energy required to perform bulk deformations, as well as improves the workable range of metallic materials. Recently, work by Ross et al. (2006) studied the electrical effects on 6Al-4V titanium during both compression and tension test (Ross, C. D., Kronenberger, T. J., and Roth, J. T., “Effect of DC Current on the Formability of 6AL-4V Titanium,” 2006 American Society of Mechanical Engineers-International Manufacturing Science & Engineering Conference, MSEC 2006-21028, 11 pp., 2006).

It is appreciated that electrical current is the flow of electrons through a material and the electrical current can meet resistance at the many defects found within materials, such as: cracks, voids, grain boundaries, dislocations, stacking faults and impurity atoms. In addition, this resistance, termed “electrical resistance”, is known and measured with the greater the spacing between defects, the less resistance there is to optimal electron motion, and conversely, the less spacing between defects, the greater the electrical resistance of the material. It was found in work by Fan, R. et al. (Fan, R., Magargee, J., Hu, P. and Cao, J., 2013, “Influence of grain size and grain boundaries on the thermal and mechanical behavior of 70/30 brass under electrically-assisted deformation.” Materials Science and Engineering: A, 574(0): 218-225) that intergranular fracture was observed by SEM (scanning electron microscope) in electrically-assisted tensile tests at lower temperatures but not in oven heated tension tests.

It is also appreciated that during loading, material deformation occurs by the movement of dislocations within the material. Furthermore, dislocations are line defects which can be formed during solidification, plastic deformation, or be present due to the presence of impurity atoms or grain boundaries, and as such, dislocation motion is the motion of line defects through the material's lattice structure causing plastic deformation.

Dislocations also meet resistance at many of the same places as electrical current, such as: cracks, voids, grain boundaries, dislocations, stacking faults and impurity atoms. Under an applied load, dislocations normally move past these resistance areas through one of three mechanisms: cross-slip, bowing or climbing. As dislocation motion is deterred due to localized points of resistance, the material requires more force to continue additional deformation. Therefore, if dislocation motion can be aided through the material, less force is required for subsequent deformation. Theoretically, this will also cause the material's ductility to be subsequently increased and a process that would afford for an increase in dislocation motion with less force would be desirable. In a recent work by Magargee et al. (Magargee, J., Fan, R. and Cao, J., “Analysis and Observations of Current Density Sensitivity and Thermally Activated Mechanical Behavior in Electrically-Assisted Deformation.” ASME Journal of Manufacturing Science and Engineering 135(6): 061022-061022, 2013), the thermal assistance through the applied current was analyzed and the sensitivity of current density on mechanical behavior was derived.

SUMMARY OF THE INVENTION

An apparatus and process for forming a piece of sheet metal while passing an electrical direct current through at least a part of the sheet metal is provided. The apparatus includes a computer numerical controlled machine that has at least one arcuate tipped tool and is operable to move the tool a predetermined distance in a predetermined direction and thereby produce an incremental deformation to a piece of sheet metal. The apparatus also has at least one electrode that is spaced a predetermined distance from the at least one arcuate tipped tool. In addition, the machine is operable to move at least one electrode in synchronization or in unison with the at least one arcuate tipped tool.

An electric current source is included and is operable to pass electrical direct current through the at least one electrode and into the piece of sheet metal during at least part of the time that the piece of sheet metal is being incrementally formed.

The at least one electrode has a tip or tip portion that is in contact with the piece of sheet metal during incremental forming thereof. The tip or tip portion can be in the form of a metal brush tip and/or an arcuate shaped tip. In some instances, the at least one electrode is at least two electrodes with a first electrode spaced a first predetermined distance and a second electrode spaced a second predetermined distance from the at least one arcuate tipped tool or a second electrode spaced to provide a predetermined force against the at least one arcuate tipped tool. In addition, the machine is operable to move the first and second electrodes in synchronization or in unison with the at least one arcuate tipped tool when the tool moves the predetermined distance in the predetermined direction.

The process for forming the piece of sheet metal includes providing the piece of sheet metal and the computer numerical controlled machine described above. The piece of sheet metal is attached to a support structure of the machine and a plurality of incremental deformations are made to the piece of sheet metal using the at least one arcuate tipped tool. In addition, here, electrical direct current is passed through the at least one electrode such that it passes through the sheet metal at a location that is proximate to where the arcuate tipped tool is in contact with the piece of sheet metal. In this manner, a desired density of electrical current can be passed through the piece of sheet metal at a desired location or distance from the arcuate tipped tool before, during and/or after the tool is making incremental deformations into the sheet metal piece.

BRIEF DESCRIPTION OF THE FIGURES

FIG. 1 is a schematic illustration of an apparatus used to cold work a metallic component while an electric current is passed through the component;

FIG. 2 is a graph illustrating the typical engineering strain versus stress for metallic components undergoing strain weakening during compressive deformation when deformed under an applied current;

FIG. 3 is a graph of engineering stress versus current density for 6Al-4V titanium alloy specimens subjected to different strain during compression testing wherein an inflection point illustrates where strain weakening begins for the alloy;

FIG. 4 is a graph of engineering stress versus strain for compression testing of 6.35 mm diameter 6Al-4V titanium alloy specimens with each specimen subjected to a different current density during the testing;

FIG. 5 is a graph of engineering stress versus strain for compression testing of 9.525 mm diameter 6Al-4V titanium alloy specimens with each specimen subjected to a different current density during the testing;

FIG. 6 is a graph of engineering stress versus strain for compression testing of 6.35 mm diameter 6Al-4V titanium alloy specimens subjected to a current density of 30 A/mm², the electric current having been initiated at different times for each specimen;

FIG. 7 is a graph of engineering stress versus strain for compression testing of 9.525 mm diameter 6Al-4V titanium alloy specimens subjected to a current density of 23.2 A/mm², the electric current having been initiated at different times for each specimen;

FIG. 8 is a graph of engineering stress versus strain for compression testing of 6.35 mm diameter 6Al-4V titanium alloy specimens subjected to a current density of 35 A/mm², the electric current having been terminated at different times for each specimen;

FIG. 9 is a graph of engineering stress versus strain for compression testing of 9.525 mm diameter 6Al-4V titanium alloy specimens subjected to a current density of 24 A/mm², the electric current having been terminated at different times for each specimen;

FIG. 10 is a graph of engineering stress versus strain for compression testing of a 6.35 mm diameter 6Al-4V titanium alloy specimen subjected to a current density of 35 A/mm², the electric current having been cycled on and off during the test;

FIG. 11 is a graph of engineering stress versus strain for compression testing of two 6.35 mm diameter 6Al-4V titanium alloy specimens subjected to a current density of 35 A/mm²and each specimen compressed with a different strain rate;

FIG. 12 is a graph of engineering stress versus strain for compression testing of a 6.35 mm diameter 6061 T6511 aluminum alloy specimen subjected to a current density of 59.8 A/mm²during compression testing;

FIG. 13 is a graph of engineering stress versus strain for compression testing of 6.35 mm diameter 7075 T6 aluminum alloy specimens with each specimen subjected to a different current density during the testing;

FIG. 14 is a graph of engineering stress versus strain for compression testing of 6.35 mm diameter C11000 copper alloy specimens with each specimen subjected to a different current density during the testing;

FIG. 15 is a graph of engineering stress versus strain for compression testing of 6.35 mm diameter 464 brass alloy specimens with each specimen subjected to a different current density during the testing;

FIG. 16 is a graph of engineering stress versus strain for compression testing of 6.35 mm diameter A2 steel specimens with each specimen subjected to a different current density during the testing;

FIG. 17 is a graph of the percentage change in energy required for deformation of an alloy as a function of applied current density to the material;

FIG. 18 is an illustration of an apparatus used to cold work a metallic component according to an embodiment of the present invention;

FIG. 19 is an illustration of an arcuate tipped tool that can be used to single point incrementally deform a sheet metal component;

FIG. 20A is an illustration of a top perspective view of a sheet metal component after being deformed by an embodiment of the present invention;

FIG. 20B is an illustration of a bottom perspective view of the sheet metal component shown in FIG. 20A;

FIG. 21A is an illustration of a top view of a sheet metal component after being deformed by an embodiment of the present invention;

FIG. 21B is an illustration of a top perspective view of a portion of the sheet metal component shown in FIG. 21A;

FIG. 22 is an illustration of a double side incremental forming apparatus according to an embodiment of the present invention;

FIG. 23 is an illustration of possible configurations of tooling for double side incremental forming;

FIG. 24 is an illustration of the effect of applied direct current on the reduction of springback on 6061 aluminum sheet metal strips;

FIG. 25A is a photograph of a 4 inch die used to bend sheet metal strips;

FIG. 25B is a photograph of sheet metal strips having been bent around the 4 inch die shown in FIG. 25A and then subjected to a 50 pound weight with and without DC electric current applied thereto;

FIG. 26 is a schematic illustration of an apparatus used to cold work a metallic component according to an embodiment of the present invention;

FIG. 27 is a top view of section A-A shown in FIG. 26 according to an embodiment of the present invention;

FIG. 28 is a top view of section A-A of FIG. 26 according to another embodiment of the present invention;

FIG. 29 is a top view of section A-A of FIG. 26 according to yet another embodiment of the present invention;

FIG. 30A is a schematic illustration of a tip portion in the form of a metal brush;

FIG. 30B is a schematic illustration of a tip portion having an arcuate shape;

FIG. 30C is a schematic illustration of a tip portion having an arcuate shape; and

FIG. 31 is a schematic illustration of an apparatus used to cold work a metallic component according to an embodiment of the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

It is postulated that, as electrons scatter off different resistant sources, for example the same resistance areas for dislocation motion, the local stress and energy field increases. This occurs since, as electrons strike the areas with a given velocity, there is an increase in the amount of kinetic energy around the resistance area due to transference from the electron as its scatters. The local Joule heating effect due to the application of electrical current can soften the resistance. Therefore, dislocations can move through the areas of resistance with increased local energy fields with less resistance. Since these areas are at a higher potential, less energy is required for a dislocation to move therethrough. In addition, the energy required to break atomic bonds as dislocations move through the lattice structure decreases.

Overall, it is postulated that the effects of current passing through a metallic material should result in a net reduction in the energy required to deform the material while simultaneously increasing the overall workability of the material by substantially enhancing its ductility. Such a postulation is supported by FIG. 17 where the percentage of total energy as a function of applied current density, with respect to a baseline test, is shown. Ideally, the mechanical energy per volume required for deformation is the area under the stress-strain curve. This energy was calculated for the curves of each material using numerical integration. Since some specimens fractured prior to completing the test, the curves were integrated to a strain slightly below the strain where the earliest fracture event occurred for any of the materials tested, which was 0.2 mm/mm. The other energy accounted for in the system is the electrical energy expended during the deformation. This energy is calculated using the relationship:

$Energy = \frac{I^{2} \cdot ρ \cdot h  \cdot t}{A_{c}}$

where I is current, ρ is resistivity, h is initial height, t is test duration and A_cis cross-sectional area. The total energy expended to deform the specimen is found by summing the mechanical and electrical energies. As shown, a small addition of electrical energy can greatly reduce the total energy required to deform the part. Moreover, as the density of the electrical energy increases, the total energy needed to deform is significantly reduced.

In an effort to more fully explain the effects and/or advantages of passing an electrical current through a metallic component while it is being formed, examples of such testing and/or processing are described in detail below.

Turning to FIG. 1, a schematic representation of an apparatus used to form and apply an electrical direct current to a metal component is shown. The electric current is provided by a direct current (DC) source 100 and deformation to a metal specimen 200 is provided by a compression source 300.

The metal specimen 200 is placed between mounts 310 which are electrically connected to the DC source 100. Upon initiation of the process, the compression source 300 is activated and a compressive force is applied to the specimen 200. While the specimen is under compression, an electrical direct current from the DC source 100 is passed through the mounts 310 and the specimen 200.

Turning to FIG. 2, a schematic representation of the stress as a function of compressive strain for the metallic specimen 200 is shown wherein a decrease in the stress required for continued strain is illustrated and afforded by passing the electric current through the specimen. This phenomenon is hereby referred to as strain weakening and has been shown to be well in excess of that which can be explained through thermal softening. In this manner, an apparatus and process for the strain weakening of a material while undergoing compressive deformation is provided.

In particular, a Tinius Olsen Super “L” universal testing machine was used as a cold forming machine and electrical direct current was generated by a Lincoln Electric R35 arc welder with variable voltage output. In addition, a variable resistor was used to control the magnitude of electric current flow. The testing fixtures used to compress metallic specimens were comprised of hardened steel mounts and Haysite reinforced polyester with PVC tubing. The polyester and PVC tubing were used to isolate the testing machine and fixtures from the electric current.

The current for a test was measured using an Omega® HHM592D digital clamp-on ammeter, which was attached to one of the leads from the DC source 100 to one of the testing fixtures 310. The current level was recorded throughout the test. A desktop computer using Tinius Olsen Navigator software was used to measure and control the testing machine. The Navigator software recorded force and position data, which later, in conjunction with MATLAB® software and fixture compliance, allowed the creation of stress-strain plots for the metallic material. The temperature of the specimens was determined during the test utilizing two methods. The first method was the use of a thermocouple and the second method was the use of thermal imaging.

The test specimens consisted of two different sizes. A first size was a 6.35 millimeter (mm) diameter rod with a 9.525 mm length. The second size was a 9.525 mm diameter rod with a 12.7 mm length. The approximate tolerance of the specimen dimensions was ±0.25 mm. After measuring the physical dimensions of a specimen 200 in order to account for inconsistency in manufacturing, the specimen 200 was inserted into the fixtures 310 of the compression device 300 and preloaded to 222 newtons (N) before the testing began. The preload was applied to ensure that the specimen had good contact with the fixtures 310, thereby preventing electrical arcing and assuring accurate compression test results. The tests were performed at a loading rate, also known as a fixture movement rate, of 25.4 mm per minute (mm/min) and the tests were run until the specimen fractured or the load reached the maximum compressive limit of 244.65 kN set for the fixtures, whichever was reached first.

The initial temperature of the specimen 200 was measured using a thermocouple and the welder/variable resistor settings were also recorded. Baseline tests were performed without electric current passing through the specimen using the same fixtures and setup as the tests with electric current. Once the specimens were preloaded to 222 N, and all of the above mentioned measurements obtained, a thermal imaging camera used for thermal imaging was activated and recorded the entire process (the specimens were coated black with high temperature ceramic paint to stabilize the specimen's emissivity). During a given test, current and thermocouple temperature measurements were also recorded by hand.

The electricity was not applied to the specimens until the force on the specimen reached 13.34 kN unless otherwise noted. It was found that the amount of strain at which time the electric current was applied affected the specimen's compression behavior and the shape of the respective stress-strain curve. After each of the tests concluded, final temperature measurements were made using the thermocouple. After cooling, the specimen was removed and a final deformation measurement taken.

A precaution was taken to ensure the accuracy of the results by testing the samples for Ohmic behavior. When metals are exposed to high electric currents, they can display non-Ohmic behavior, which can significantly change their material properties. Therefore, tests were conducted with high current densities to ensure that the metallic material tested was still within its Ohmic range. This was accomplished by applying increased current densities to a specimen, and measuring the corresponding current and voltage. Using the measured resistivity of the metallic materials, it was verified that the materials behaved Ohmically, that is the Ohm's Law relationship was obeyed.

Testing Results

Initially, tests were conducted in order to find the current density needed to cause strain weakening behavior to occur with 6Al-4V titanium. This density was determined by plotting the decrease in strength for the material with an increase in current density. As shown in FIG. 3, wherein each line represents a constant strain, the stress required to obtain a particular strain as a function of current density was plotted. The graph shows the degree to which the strength of the material decreases as the current density increases. In addition, the point where strain weakening begins is the inflection point noted on the graph and shown by the arrow. It is appreciated that this process can be used to estimate the current density at which other metallic materials will exhibit strain weakening.

Turning to FIG. 4, strain weakening exhibited by 6Al-4V titanium is shown. Starting with a current density of approximately 25 amps per square millimeter (A/mm²) and performing tests with higher current densities, a decrease in stress for continued increase in strain was observed at yield points of approximately 0.04 mm/mm strain for 6.35 mm diameter specimens. A comparative test run with no electric current is also shown in the figure for comparison. Thus the unique phenomena of obtaining further deformation of a metallic material with a decrease in stress is shown in this plot, where the baseline material fractured between 0.3 and 0.4 strain, while the specimens deformed under the applied current never fractured. Furthermore, it is seen that the higher the current density, the earlier the material yields and the more the overall ductility or strain at fracture increases. This decrease in force for continued deformation of the material is well suited for forming parts and components. Similar results are shown in FIG. 5 wherein specimens having a diameter of 9.525 mm were tested.

The effect of initiating the electric current at different times or strains during the compression test is illustrated in FIG. 6 for 6.35 mm diameter specimens and FIG. 7 for 9.525 mm diameter specimens. A current density of 30 A/mm²was used for the 6.35 mm diameter specimens and 23.2 A/mm²for the 9.525 mm diameter specimens. As shown in FIG. 6, specimens where the electric current was initiated at 0.89 kN, 2.22 kN, 13.34 kN and 22.24 kN during the compression testing exhibited behavior that was a function of when the electric current started. For example, the sooner the electric current was applied to the specimen, the lower the yield point of the material. In addition, the sooner the electric current was initiated, the greater the amount of strain weakening exhibited by a particular specimen. The same is true for the 9.525 mm diameter specimens as illustrated in FIG. 7.

It is appreciated that some of these effects can be contributed to temperature, since the sooner the electric current was initiated, the faster and hotter a specimen became. However, it has been established that the effect of an applied current during deformation is greater than can be explained through the corresponding rise in workpiece temperature. It is further appreciated that the amount of work hardening imposed on the specimen can vary as a function of the time load when the electric current is initiated.

The effect of removing the electric current during the testing process was also evaluated. Turning to FIG. 8, a plot of 6.35 mm diameter specimens compression tested with no electricity and with electricity applied during the entire test is shown for comparison. In addition, the two plots wherein the electric current was terminated at a total deformation of 2.032 mm and 3.048 mm are shown. For the 9.525 mm diameter specimens, the electric current was terminated at a total strain of 3.048 mm and 4.064 mm (see FIG. 9). These figures illustrate that the sooner the electric current is terminated the sooner the specimens stop exhibiting strain weakening behavior. In addition, when the electric current is terminated the slope of the stress versus strain curve is steeper than if the electric current is applied to a specimen for the entire test. Furthermore, when the electricity was discontinued early in the test, the material once again was found to fracture.

It is appreciated that the effects of initiating and/or terminating the electric current at different points along a compression/deformation process can be used to enhance the microstructure and/or properties of materials, components, articles, etc. subjected to deformation processes. For example, in some instances, a certain amount of work hardening within a metal component would be desirable before the onset of the strain weakening were to be imposed. In such instances, FIGS. 6 and 7 illustrate that work hardening could be imposed on a component by initiating the electric current through the workpiece after plastic deformation has begun. In other instances, a certain amount of work hardening imposed on a workpiece after or towards the end of the deformation process could be desirable. As such, FIGS. 8 and 9 illustrate how the termination of the electric current passing through the component at different times or strains of the deformation process result in different amounts of work hardening in the sample. In this manner, physical and/or mechanical properties, illustratively including strength, percentage of cold work, hardness, ductility, rate of recrystallization and the like, of a formed component can be manipulated.

Turning now to FIG. 10, the effect of the electric current on the enhanced forgeability of 6AL-4V titanium was demonstrated by passing a current density of 35 A/mm²through the sample and cycling the current during the test. The electricity was initiated at a force of 13.34 kN and then cycled on and off approximately every 1 mm of deformation up to a total of 4 mm, at which point the electricity remained off until the test was completed. As indicated in the figure, it is visible that the electric current was terminated at approximately 0.225 mm/mm and then reapplied at 0.290 mm/mm. In addition, it is apparent that when the electric current was terminated, the sample exhibited work hardening stress-strain behavior evidenced by an increase in stress for continued plastic deformation. As such, cycling the electric current during compression forming can also afford for the control and manipulation of a components physical and/or mechanical properties.

The effect of varying the strain rate during compression testing is shown in FIG. 11, with a 6.35 mm diameter specimen tested at platen speeds of 12.7 and 83.3 mm/min. The electric current was applied to the specimens at a load of 4.45 kN and remained on during the entire test. As illustrated in FIG. 11, the approximate amount of time the sample exhibits strain weakening is equivalent for both strain rates, however the initiation of strain weakening occurred sooner for the lower strain rate while the end of strain weakening behavior occurred later for the higher strain rate. As such, the amount of work hardening produced in a component before strain weakening occurs can be further manipulated by the strain rate.

Strain weakening behavior via electric current has been demonstrated by other alloys as illustrated in FIGS. 12-16. For example, FIG. 12 shows a stress-strain curve wherein a 6061 T6511 aluminum specimen underwent compression testing with a current density of 59.8 A/mm²applied thereto. As shown in this figure, at a strain of approximately 0.10 mm/mm a decrease in stress was required for additional deformation to occur. Likewise, FIGS. 13-15 illustrate similar strain weakening behavior for 7075 T6 aluminum with a 90.1 A/mm²current density applied thereto, C11000 copper (92.4 A/mm²) and 464 brass (85.7 A/mm²).

The inducement of strain weakening using the current process of the present invention can also be applied to ferrous alloys. FIG. 16 illustrates an A2 tool steel which has been subjected to a number of different current densities while undergoing compression testing. As shown in this figure, at a current density of 45.1 A/mm², the A2 tool steel exhibited a decrease in stress required for an increase in strain after a yield point at approximately 0.02 mm/mm. Thus it is apparent that the process wherein electric current is used to induce strain weakening and control/manipulate physical and/or mechanical properties can be applied to a variety of metallic materials.

Use of electrical-assisted forming can also be used in producing components as illustrated by a single point incremental forming (SPIF) machine 320 having an arcuate tipped tool 322 as shown in FIGS. 18 and 19. For the purposes of the present invention the term “arcuate tipped tool” includes any tool with a curved shaped tip, illustratively including tools with a round shaped tip, spherical shaped tip and the like. The forming machine has a support structure 330 onto which a piece of sheet metal 210 can be placed. In some instances, the support structure 330 has a clamping structure 332 that can rigidly hold an outer perimeter 212 of the piece of sheet metal 210 and leave a portion 214 of the sheet metal 210 unsupported. In addition, the arcuate tipped tool 322 may or may not have a spherical shaped head 321 with a shaft 323 extending therefrom.

Also included with the forming machine 320 is the electrical current source 100 that is operable to pass electrical direct current through the piece of sheet metal 210. In some instances, the electrical direct current passes through the arcuate tipped tool 322 to the piece of sheet metal 210. In fact, the electrical current can pass down through the arcuate tipped tool 322, pass through a minimal amount of the sheet metal 210 where deformation is occurring and then exit the sheet metal through a probe (not shown) that is offset from the tool. In this manner, the entire workpiece does not have to be energized, i.e. have electrical current passing through it. It is appreciated that the single point incremental forming and/or electrical current can be applied to the sheet metal 210 during cold, warm and hot forming operations.

The forming machine 320 can be a computer numerical controlled machine that can move the arcuate tipped tool 322 a predetermined distance in a predetermined direction. For example, the forming machine 320 can move the arcuate tipped tool 322 in a generally vertical (e.g. up and down) direction 1 and/or a generally lateral (e.g. side to side) direction 2. In the alternative, the support structure 330 can move the piece of sheet metal 210 in the generally vertical direction 1 and/or the generally lateral direction 2 relative to the arcuate tipped tool 322. The arcuate tipped tool 322 can be rotationally fixed, free to rotate and/or be forced to rotate. After the piece of sheet metal 210 has been attached to the support structure 330, the arcuate tipped tool 322 comes into contact with and makes a plurality of single point incremental deformations on the piece of sheet metal 210 and affords for a desirable shape to be made therewith.

During at least part of the time when the arcuate tipped tool 322 is producing the plurality of single point incremental deformations on the piece of sheet metal 210, the electrical direct current can be made to pass through the piece of sheet metal. It is appreciated that in accordance with the above teaching regarding passing electrical direct current through a metal workpiece, that the force required to plastically deform the piece of sheet metal is reduced. In addition, it is appreciated that the amount of plastic deformation exhibited by the piece of sheet metal before failure occurs can be increased by passing the electrical direct current therethrough.

It is further appreciated that the amount of springback exhibited by the plastic deformation of the piece of sheet metal is reduced by the electrical direct current. In some instances, the amount of springback is reduced by 50%, while in other instances the amount of springback is reduced by 60%. In still other instances, the amount of springback can be reduced by 70%, 80%, 90% or in the alternative greater than 95%. The arcuate tipped tool may be rotationally fixed, freely rotating or forced to rotate. In addition, this process provides for a die-less fabrication technique ideally suited for the manufacture of prototype parts and small batch jobs with FIGS. 20 and 21 illustrating example shapes made using an embodiment of the present invention.

Having discussed the effects of passing an electrical current through a metallic workpiece and its use in SPIF above, the present invention discloses a process for producing prototype and/or one-of-a-kind metallic components by forming a sheet metal component using an electrical-assisted double side incremental forming (EADSIF) machine that also provides a source of electrical current to the component during deformation thereof. The process passes an electrical current through the sheet metal component during at least part of the forming operation and can control the work hardening of the sheet metal component, reduce the force required to obtain a given amount of deformation and/or reduce the amount of springback typically exhibited by the component. As such, the present invention has utility as a manufacturing process. For the purposes of the present invention, the term “work hardening” is defined as the strengthening of a component, specimen, etc., by increasing its dislocation density and such type of strengthening is typically performed by cold forming the component, specimen, etc. The terms “metal” and “metallic” are used interchangeably and deemed equivalent and include materials known as metals, alloys, intermetallics, metal matrix composites and the like, and the term “springback” is defined as the amount of elastic recovery exhibited by a component during and/or after being subjected to a forming and/or deformation operation.

The process can include forming a piece of sheet metal with a plurality of double side incremental deformations by a pair of arcuate tipped tools located on opposite sides of a piece of sheet metal and with one or both of the tools being fixed, freely rotating, or undergoing forced rotation while electrical direct current is passing through the piece of sheet metal at least part of the time it is being formed. The electricity can be applied through any portion of the sheet metal when it is being applied. In addition, the plurality of double side incremental deformations can be afforded by a computer numerical controlled machine that is operable to move one or both of the arcuate tipped tools a predetermined distance in a predetermined direction. In the alternative, a support structure provided to rigidly hold at least part of the sheet metal component can move the sheet metal component a predetermined distance in a predetermined direction. In any event, the arcuate tipped tools come into contact with and push against the sheet metal component from opposite sides to produce an incremental deformation, with the plurality of incremental deformations producing a desired shape out of the component. In some instances, the electrical direct current is applied to the component before, during and/or after the forming of the component has been initiated and/or before, during and/or after the forming has been terminated.

Turning now to FIG. 22, a schematic illustration of an electrical-assisted double side incremental forming (EADSIF) machine is shown generally at reference numeral 10. The EADSIF machine can have one or more clamps 150 and at least a first arcuate tipped tool 330 and a second arcuate tipped tool 332. As shown in FIG. 22, the arcuate tipped tools 330, 332 can be oppositely disposed from each other with a sheet metal component 210 therebetween and may or may not be offset from each other vertically and/or laterally. Similar to the SPIF machine 320 shown in FIG. 18, the EADSIF machine 10 can have an electrical current source (not shown) that is operable to pass electric direct current through a piece of sheet metal 210. In some instances, the electrical direct current passes through at least one of the arcuate tipped tools 330, 332 to the piece of sheet metal 210.

The EADSIF machine 10 can be computer numerical controlled such that at least one of the arcuate tipped tools 330, 332 can be moved a predetermined distance in a predetermined direction. In addition, the sheet metal piece 210 can be clamped around its periphery using the one or more clamps 150 and deformed by the pair of arcuate tipped tools 330, 332, one on each side of the sheet 210. The upper or top arcuate tipped tool 330 can have three or up to six degrees of freedom, while the bottom or lower tool 332 can be moved passively with the top tool 330, or in the alternative, be independently controlled with having up to six degrees of freedom.

The motion of the two tools 330, 332 along a prescribed tool path can incrementally deform the sheet 210 into a three-dimensional part and thereby satisfy most, if not all, engineering applications made of thin sheet metals. It is appreciated that since the deformation occurs locally, the forming force is significantly decreased from traditional sheet metal forming operations such as stamping. In some instances, the electrical direct current can pass through only one of the arcuate tools 330, 332, while in other instances, the electrical current can pass through both of the tools 330, 332.

Turning now to FIG. 23, the relative positioning of two forming tools can have a variety of orientations relative to each other. As such, tool path generation form double side incremental forming can be more complicated than with single point incremental forming. In some instances, the relative position and orientation of the arcuate tipped tool 330, 332 can be based on a mechanics analysis of the amount of compressions/stretch/bending that occurs locally within the sheet metal piece 210, compensation for any elastic deformation of insulation materials and/or considering any improvement in material formability due to the electrical assistance.

As stated above, providing electrical direct current through the sheet metal piece 210 can reduce springback. For example and for illustrative purposes only, FIG. 24 provides an illustration and a plot of percent of baseline springback as a function of current density for electrical current that has passed through the metal strips shown in the photograph. As shown in the illustration, strips of sheet metal were bent around an insulated die (four inch diameter) and a single pulse of electrical current was applied to the sheet metal strip prior to releasing the specimen from the die. As the current density was increased, the springback was reduced until all of the springback was eliminated at a current density of 120 A/mm². The trend of springback as a function of applied current density is shown in the graph.

The use of applied electrical current to sheet metal components can also provide for reduced energy remanufacturing. For example and for illustrative purposes only, FIGS. 25A and 25B provide an illustration on how the use of applied electrical current to sheet metal strips affords for the return of a plastically deformed piece of material to its original shape. In particular, strips of sheet metal were bent around a four inch diameter die as shown in FIG. 25A and then released. The released strip of sheet metal had a generally new shape as shown by the top strip in FIG. 25B. Thereafter, a 50 pound weight was placed on top of a bent metal strip, so as to straighten the bent material, and then subsequently removed. For originally bent metals strips that were not subjected to electrical current, the 50 pound weight did produce some deformation as shown by the middle metal strip in FIG. 25B. However, in cases where an electric pulse was applied while the specimens were being flattened with the 50 pound weight, the springback was eliminated as shown by the bottom strip in FIG. 25B. In this manner, used or prior plastically deformed sheet metal can be reshaped and reused without having to remelt the material and reproduce sheet metal. As such, large savings in time, energy, equipment, etc. can be provided by passing an electrical current through a piece of sheet metal.

Another embodiment for an apparatus used to form a metallic component with electrical-assistance is shown in FIG. 26. The apparatus shown in FIG. 26 is similar to the SPIF machine 320 shown in FIG. 18 with the addition of at least one electrode 400. As shown in the figure, the electrode 400 is electrically connected to the electrical current source 100 that is operable to pass electrical direct current through the at least one electrode 400 and into the piece of sheet metal 210. Also similar to the discussion above, the electrical current can be passed through the at least one electrode 400 and the piece of sheet metal 210 before, during and/or after the arcuate tipped tool 322 produces the plurality of single point incremental deformations on the piece of sheet metal 210. It is appreciated that the at least one electrode 400 can be attached to, but electrically insulated from, a spindle that the arcuate tipped tool 322 is attached to, however this is not required. Stated differently, the at least one electrode 400 can move with in unison with the arcuate tipped tool 322 by being attached to and moving with the spindle that holds the tool 322. In the alternative, the at least one electrode 400 can be attached to a separate structure, robotic arm, etc., that moves in unison with the arcuate tipped tool 322.

Referring now to FIGS. 27-29, various embodiments of the electrode 400 are shown and discussed. In particular, FIG. 28 shows an embodiment in which the electrode 400 is a pair of electrodes 404 that are spaced apart from the center of the arcuate tipped tool 322 at a distance d1, or in the alternative a distance d2, from the outer surface of the tool 322. The electrodes 404 have a width W that is selected and/or designed such that a desired electrical current density is passed through the sheet metal 210 at the predetermined distance d1 or d2 from the tool 322. For example, in some instances at least one of the electrodes 404 is less than 2 inches from the outer surface of the tool 322 (d2), or in the alternative less than 2 inches from the center of the tool 322 (d1). In other instances, at least one of the electrodes 404 is less than 1 inch from the outer surface of the tool 322 (d2), or in the alternative less than 1 inch from the center of the tool 322 (d1). As such, it is appreciated that the at least one electrode 400 is not the same as the clamping structure 332 shown in the figure.

It is appreciated that the apparatus shown in FIG. 26 can have only one of the electrodes 404, or in the alternative three, four, or more electrodes, in relatively close proximity at a predetermined distance from the tool 322. In addition, FIG. 27 illustrates that the electrodes 404 are both equally spaced from the tool 322, however this is not required.

FIG. 28 illustrates a cylindrical shaped electrode 402 that surrounds the arcuate tipped tool 322 with a predetermined distance d1 being present between the center of the arcuate shaped tip 321. In the alternative, the cylindrical shaped electrode 402 can be a predetermined distance d2 from an outer diameter or outer surface of the arcuate tipped tool 322. The width W of the electrode 402 is selected such that a desired electrical current density is passed through the sheet metal 210 at the distance d1, or in the alternative distance d2, from the tool 322.

Looking now at FIG. 29, a pair of arc shaped electrodes 406 are shown. The electrodes 406 are spaced a predetermined distance d1, or in the alternative d2, from the arcuate tipped tool 322. It is appreciated that the doubled-headed arrows in FIGS. 27-29 illustrate that the electrode 402, the one or more electrodes 404, and the one or more electrodes 406 can rotate with the arcuate tipped tool during deformation of the sheet metal 210. In the alternative, the electrodes are not required to rotate with the tool but can remain stationary with respect to rotation.

It is also appreciated that the electrodes move in synchronization or in unison with the tool 322 such that the desired distance between the electrode and the arcuate tipped tool 322 is maintained while the tool performs its plurality of incremental deformations to the sheet metal 210. However, the exact distance between the one or more electrodes and the arcuate tipped tool 322 can change with time depending on the desired distance between the electrode and the tool at any given time during the deformation process. Furthermore, the electrodes 402-406 can move in an up and down direction as illustrated by the double-headed arrow 3 in FIG. 26 in order to ensure that contact with the sheet metal piece 210 is maintained. For example, the electrodes 402-406 can be spring loaded in an up and down direction such that a constant force is applied to the electrodes in order to ensure that a tip thereof maintains contact with the sheet metal 210.

Referring to FIG. 30, detailed illustrations of tip portions for the electrode 400 are shown. In particular, a tip portion 410 can be in the form of a metal brush made from a plurality of metallic wires as shown in FIG. 30A. It is appreciated that the metal brush 410 allows for the electrode 400 to maintain electrical contact with the piece of sheet metal 210. In the alternative, the electrode can have a tip portion 412 that is arcuate in shape as shown in FIG. 30B and adequately slides and is in contact with the sheet metal 210 while the arcuate tipped tool 322 performs its plurality of incremental deformations. Finally, the electrode 400 can have an arcuate shaped tip 414 as shown in FIG. 30C which provides an increase in surface area in contact with the sheet metal 210.

FIG. 31 provides another embodiment of an apparatus for performing incremental deformation at reference numeral 30. The apparatus 30 is similar to the apparatus shown in FIG. 22 except for the addition of the one or more electrodes 400. In addition, it is appreciated that the electrodes can be on opposite sides of the piece of sheet metal 210 and work or function in a similar manner as discussed above with respect to FIG. 26.

The foregoing drawings, discussion and description are illustrative of specific embodiments of the present invention, but they are not meant to be limitations upon the practice thereof. Numerous modifications and variations of the invention will be readily apparent to those of skill in the art in view of the teaching presented herein. It is the following claims, including all equivalents, which define the scope of the invention.

	Number	Date	Country
Parent	13221304	Aug 2011	US
Child	14293270		US
Parent	12194355	Aug 2008	US
Child	13221304		US
Parent	12117970	May 2008	US
Child	12194355		US

APPARATUS FOR ELECTRICAL-ASSISTED INCREMENTAL FORMING AND PROCESS THEREOF

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CPC

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