die design for flashless forging of complex parts
TRANSCRIPT
Die design for ¯ashless forging of complex parts
Victor Vazquez, Taylan Altan*
ERC for Net Shape Manufacturing, The Ohio State University, Columbus, OH 43210 USA
Abstract
In conventional hot forging of connecting rods, the material wasted to the ¯ash accounts approximately 20±40% of the original
workpiece. In order to reduce the cost of forged products, the forging must be performed in a closed cavity to obtain near-net or net shape
parts. In ¯ashless forging, the volume distribution of the preform must be accurately controlled to avoid overloading the dies and to ®ll the
cavity. Additionally, the preform must be simple enough to be mass-produced.
This study deals with the preform design for ¯ashless forging of a connecting rod and introduces a new tooling concept for forging of
complex parts with a controlled amount of ¯ash. In both studies the use of process simulations has been helpful in the performance of
several iterations without requiring the construction of expensive tooling. # 2000 Elsevier Science S.A. All rights reserved.
Keywords: Die design; Flashless forging; Tool design
1. Introduction
If the weight of a connecting rod (see Fig. 1) can be
reduced while increasing its strength, an automobile's fuel
ef®ciency will be improved. Currently, steel connecting rods
are used in passenger cars. However, some manufacturers
have attempted to use alternative lighter materials. Recently,
various composite materials based on aluminum have been
considered, but not yet successfully adopted, for automotive
engines. The main reasons are that these materials are not
strong enough, or when strong enough, are too expensive.
Flashless forging offers the possibility of producing alu-
minum composite connecting rods at competitive costs. The
design of ¯ashless forging processes is more complex than
the design of conventional closed die forging with ¯ash.
Therefore, in order to accelerate the development of the
manufacturing process as well as to reduce the development
costs, a new design method must be developed and applied.
The ®nite element method (FEM) offers the possibility to
design the entire manufacturing process on a computer. This
leads to a reduction of the cost and time in process and tool
design, tool manufacturing, and die try-out. In addition, it is
possible to modify the process conditions in the simulation
to ®nd the best manufacturing conditions for a product.
1.1. Forging of connecting rods
In the forging of connecting rods, three main methods are
employed. The ®rst method consists of making a rough
preform from a non-porous billet and hitting it several times
in a press until the ®nal shape is obtained (left of Fig. 2).
This method results in 20±40% of the material to be wasted
as ¯ash. A major advantage of the closed-die forging with
¯ash is that the volume of the preform can vary within a
wider range than for ¯ashless forging. This makes it easier to
continuously manufacture products with the same quality.
However, a trimming process is necessary to remove the
existing ¯ash.
The second method is net shape ¯ashless forging (right of
Fig. 2). During this process the preform is totally enclosed in
the die cavity so that no ¯ash formation is allowed. There is
no material waste as in impression forging. However, tight
volume control of the preform is necessary to insure ®lling
of the cavity and to avoid overloading the tooling. The third
method, which is widely used, is hot forging of powder
metallurgy preforms. This method yields virtually no mate-
rial waste and produces near-net shape products. However,
the metal powder is expensive compared to conventional
materials.
In principle, forging operations are non-steady state pro-
cesses, in which the deformation of the material takes place
under three-dimensional stress and strain conditions. The
material ¯ow depends mainly on the following [1]:
Journal of Materials Processing Technology 98 (2000) 81±89
* Corresponding author. Tel.: +1-641-292-9267; fax: +1-614-292-7219.
E-mail address: [email protected] (T. Altan)
0924-0136/00/$ ± see front matter # 2000 Elsevier Science S.A. All rights reserved.
PII: S 0 9 2 4 - 0 1 3 6 ( 9 9 ) 0 0 3 0 8 - 8
1. geometry of the cavity;
2. geometry of the flash opening;
3. initial and intermediate billet geometry;
4. percentage of flash;
5. heat transfer between the tooling and the billet.
Thus, the requirements to perform a successful ¯ashless-
forging process are:
1. The volume of the initial preform and the volume of the
cavity at the end of the process must be the same.
2. There must be neither a local volume excess nor a
shortage, which means that the mass distribution and
positioning of the preform must be very exact.
3. If there is a compensation space in the dies, the real cavity
must be filled first.
This study deals with the preform design for ¯ashless
forging of a connecting rod and introduces a new tooling
concept for forging of complex parts with a controlled
amount of ¯ash. In both studies the use of process simula-
tions has been helpful in the performance of several iterations
without requiring the construction of expensive tooling.
2. Tool and process design for flashless forging of aconnecting rod
The design of ¯ashless forging processes is more complex
than the design of conventional closed die forging with ¯ash.
The ®nite element method (FEM) and the physical modeling
techniques offer the possibility to accelerate the develop-
ment of the manufacturing process as well as to reduce
the development costs associated with the design of the
entire manufacturing process. In addition, it is possible to
perform several iterations to modify the process parameters
to determine the best manufacturing conditions for a forged
product.
2.1. Physical modeling applied to preform design
Before 3D FEM simulations were practical, physical
modeling experiments and 2D FEM simulations were used
[2] to de®ne a preform for the ¯ashless forging of a con-
necting rod. 3D FEM simulations of the ¯ashless forging of a
connecting rod were attempted [3] but were unsuccessful
due to limitations in remeshing.
2.1.1. Physical modeling experiments
Physical modeling experiments were performed for the
¯ashless forging of a connecting rod using plasticine billets
and aluminum tooling (see Fig. 3) [2]. The experiments
were performed with the ERC/NSM ®ve-ton multi-action
press. The main objective of the plasticine experiments was
to ®nd a preform geometry that would result in complete
tilling of the die cavity.
The volume distribution in the connecting rod was
obtained by cutting several transverse sections and comput-
ing the area of each one. These values are plotted in Fig. 4 as
the cross-section area versus the length of the connecting
rod. The area under the curve represents the volume dis-
tribution of the ®nal shape of the connecting rod. Based on
these results an axisymmetric preform was designed. The
preform suggested in [2] is shown in Fig. 5. This preform
was modi®ed based on the physical modeling experiments.
The ®nal plasticine preform and connecting rod is shown in
Fig. 6 (Preform I).
Fig. 1. Connecting rod.
Fig. 3. Aluminum tooling for physical modeling of flashless forging of
connecting rod.
Fig. 2. Closed-die forging with and without flash.
82 V. Vazquez, T. Altan / Journal of Materials Processing Technology 98 (2000) 81±89
2.2. 3D FEM simulation of flashless forging process
In order to verify the applicability of the new FEM code
DEFORM 3D to the optimization of the preform design, a
simulation of the real connecting rod was performed using
Preform I as de®ned in previous studies [2,3].
An upsetting step of the initial preform had to be carried
out to start the whole forging process, because the pin-end of
the initial preform was too big to ®t into the die cavity. This
simulation is performed at hot forging temperature (see
Fig. 7). The relevant data for this simulation are shown in
Table 1.
The simulation of the ¯ashless forging was carried out
using one upper punch, one die, and the previously deformed
preform as shown in Fig. 8.
The material ¯ow of the connecting rod forging process is
shown in Fig. 9. Fig. 10 shows the contact condition
between the crank-end portion of the billet and the tooling
at the end of the forging. It can be seen from this ®gure that a
relatively large cavity remains at the upper surface of the
crank journal ring (marked as `*' in Fig. 10). The I-beam
section is formed from the ends, thus the metal ¯ow for this
section is not under plane strain.
It was concluded from these results that to optimize the
initial geometry of the preform the following problems have
to be solved [4]:
1. For the crank-end section, it is necessary to redesign the
preform so that it ®lls the cavity completely and
uniformly.
2. For the pin-end section, it is necessary to control the
initial volume distribution and transfer the excessive
volume to other features of the product.
3. For the I-beam section, it is required to determine the
diameter for which plane strain flow could be achieved.
Fig. 4. Axisymmetric plasticine preform.
Fig. 5. Sketch of Preform I of the connecting rod [4].
Fig. 6. Plasticine preform and connecting rod [2].
Fig. 7. Effective strain distribution after upsetting.
Table 1
Input data for the upsetting process
Simulation parameter
Billet material Al 2618
Punch velocity 20 mm/s
Stroke 4.5 mm
Simulation mode Isothermal
Simulation steps (NSTEP) 90
Fig. 8. FEM model for the forging of the connecting rod [4].
V. Vazquez, T. Altan / Journal of Materials Processing Technology 98 (2000) 81±89 83
2.3. Optimization of the preform geometry
It would be very dif®cult to optimize the whole geometry
of the preform at once, since the preform shape is relatively
complex and has a lot of shape parameters as shown in
Fig. 5. Hence, the workpiece was divided into three sections:
crank-end section, pin-end section, and I-beam section. Each
section was optimized independently. This optimization
procedure was adopted for the following reasons [4]:
� Since the I-beam section deforms nearly under plane
strain conditions, it is assumed that the deformation of
the large-end section and that of small-end section do not
strongly interfere with each other.
� The number of shape parameters is reduced and the
optimization process becomes easy to handle.
� The simulation time is reduced by working with a smaller
model.
The seven shape parameters for the crank-end were
reduced to three independent parameters and four dependent
parameters. Three preform designs were selected from the
combinations of parameters.
The top-view of the material ¯ow for the crank-end
preforms is shown in Fig. 11. The shaded area indicates
contact between the billet and the tools. It is clear that the
selection of the geometrical parameters affect signi®cantly
the metal ¯ow.
Similarly for the pin-end, three preforms were de®ned.
The top-view of the ®nal shape achieved for each preform is
shown in Fig. 12. The deformation pattern of the pin-end is
not sensitive to the initial geometry of the preform because it
is completely formed before the forging process for the
whole connecting rod is completed.
There are three parameters in the connecting I-beam
section: diameter d3 and segment lengths s4 and s5, as
shown in Fig. 5. The area of a cross-section of the I-beam
part calculated by I-DEAS was 42.637 mm2. Hence, assum-
ing that the material of this part is ¯ows under plane strain
conditions the initial diameter d3 of the connecting I-beam
section was set to 7.37 mm.
2.4. FE simulation with the optimized preform
Evaluating the results obtained from the optimization
method, a new preform design is proposed (Preform II),
shown in Fig. 13. A second 3D FEM simulation was per-
formed with this preform design, and was compared with the
earlier results. The dimensions of the new preform are
shown in Table 2.
The material ¯ow of the connecting rod forging process
with Preform II resulted as follows: the pin-end section is
formed completely, the I-beam section ¯ows nearly under
plane strain conditions, and the crank-end section is ®lled
Fig. 9. Material flow in forging of the connecting rod.
Fig. 10. Contact condition with the tools at the crank-end section: (�)
contact, (*) no contact.
Table 2
Shape parameters of Preform II, mm
s1 s2 s3 s4 s5 s6 s7 s8 d1 d2 d3 d4 d5
14.50 6.82 20.18 18.50 13.50 7.19 7.11 4.70 9.00 20.00 7.37 15.75 7.00
84 V. Vazquez, T. Altan / Journal of Materials Processing Technology 98 (2000) 81±89
almost completely. It was concluded that fair results may be
obtained with the design for Preform II.
2.5. Manufacturing the preform
The preform suggested in the previous section could
be manufactured by cross rolling. However, variations in
the cross-rolling process may affect the required dimensions
of the initial preform for the ¯ashless forging process. In
order to verify these points, further investigations of the 3D
FEM simulation or physical modeling experiments are
needed.
3. Die design for forging of connecting rod withcontrolled amount of flash
As discussed above, in the ¯ashless forging of the con-
necting rod, the material savings could be signi®cant. How-
ever, the manufacturing of preforms with a tight controlled
volume may increase the manufacturing cost. An alternative
die design has been proposed at the ERC/NSM. This die
design consist in a closed die that would be able to produce
forgings with a controlled amount of ¯ash (5%).
3.1. Research objectives
1. Design a tooling concept that can save material by
allowing the formation of only a small amount of ¯ash.
Optimize the tooling design with the aid of ®nite
element simulations.
2. Establish guidelines and procedures to design blockers
and preforms in order to accelerate the development of
the production process of a forged part.
Fig. 11. Material flow for the preforms defined for the optimization of the crank-end.
Fig. 12. Final stage deformed billets of the pin-end section in top view
(XY plane).
Fig. 13. Comparison of the shape parameters of Preform II with that of
Preform I.
V. Vazquez, T. Altan / Journal of Materials Processing Technology 98 (2000) 81±89 85
3.2. Tool design concept for forging of connecting rod with
a controlled amount of flash
Several researchers [3±5] conducted investigations at the
ERC/NSM on ¯ashless forging of connecting rods. These
investigations were performed with the objective of forging
an aluminum connecting rod without ¯ash. However, to
achieve ¯ashless forging it would be necessary to have very
tight tolerance control in the manufacturing of the preform.
That may not be economically feasible. It was concluded
that the formation of ¯ash should be allowed in order to ®ll
the cavity and produce connecting rods with an economical
process.
The locus of this investigation was to develop a hot
forging tooling that will allow the forging of a connecting
rod with a controlled amount of ¯ash. It has been established
that 5% of material waste may be reasonable under the
present production conditions. Thus, this tooling should be
simple enough to be used in mass production.
The proposed tooling concept consists of three different
parts (Fig. 14): (1) punch, (2) outer die, and (3) bottom die.
The tooling works as follows:
� Stage 1: The blocker is inserted in the bottom die.
� Stage 2: The ram moves down and closes the cavity. The
outer die is in contact with the bottom die. In this stage the
blocker does not come into contact with the outer die
walls. There is no workpiece deformation during this
stage.
� Stage 3: The punch keeps moving down with the ram and
the deformation starts. The workpiece fills the cavity
flowing in the direction of least resistance. When the
cavity is filled, or almost filled, the material starts to fill
the flash gap. The material flowing into the flash helps to
compensate for inaccuracies in the control of the volume
of the blocker.
Since the ¯ash is in a restricted area, the die/workpiece
contact stresses increase at the ¯ash-land entrance. This
allows ®lling of the cavity without overloading the tooling.
A 3D model was designed using I-DEAS (Fig. 15) from
the tooling concept described above. This model was based
on the tooling used in [3], for the simulation of ¯ashless
forging of a connecting rod. This tooling was modi®ed in
order to allow the formation of ¯ash. Some draft and ®llets
were added in order to permit the ejection of the part after
forging and to decrease the load on the tooling.
3.3. Two-dimensional simulations of the I-beam section
In order to validate the previously described tooling
concept two-dimensional simulations using DEFORM-2D
were performed for the I-beam section of the connecting rod.
Previous studies [4] showed that the three-dimensional
simulations are time consuming.
In order to save computation time isothermal plane strain
simulations were conducted. In this simulations the position
and thickness of the ¯ash gap were varied. These simulations
helped to de®ne an optimum tooling geometry. Then some
non-isothermal simulations were carried out.
In addition, isothermal simulations with a conventional
closed die tooling with ¯ash were performed. These simula-
tions were performed with a ¯ash amount of 18%, which is
common for this kind of forging. These simulations were
used to compare forging with controlled ¯ash and conven-
tional forging with ¯ash.
3.3.1. Simulation parameters
Three ¯ash locations were selected in the tooling
(Fig. 16):
1. Flash 2.5 mm above the web symmetry plane (Geometry
I).
2. Flash gap in the web symmetry plane (Geometry II).
3. Flash 2.5 mm below the web symmetry plane (Geometry
III).
Fig. 14. Tooling concept for forging with controlled flash.
Fig. 15. Exploded view of the tooling for controlled flash forging.
86 V. Vazquez, T. Altan / Journal of Materials Processing Technology 98 (2000) 81±89
These three locations were selected because they are the
probable extreme ¯ash locations in the tooling. The ¯ash
thickness varied from 0.4 to 0.8 mm (Fig. 16). The para-
meters used to simulate the forgings with the controlled ¯ash
are given in Table 3.
The parameters used to simulate the conventional closed
die forging with ¯ash are the same as the ones used for the
previous simulations except that the stroke was 3.66 mm and
the ¯ash amount was 18%.
All the simulations started with 300 elements. When the
workpiece started ®lling the ¯ash gap, re-meshing was
performed. The re-meshing was done with 900 elements
with a high-density ¯ash entrance.
The load-stroke curve shown in Fig. 17 can be divided
into four zones where the workpiece behaves in different
way:
� Zone I: This zone covers roughly 70% of the stroke. In
this zone the workpiece is upset between the punch and
the bottom die.
� Zone II: This zone covers up to 75% of the stroke. In this
zone the workpiece sides touch the die walls. The load
increases since material movement is restrained.
� Zone Ill: This zone covers up to 95% Of the stroke. In this
zone the workpiece fills the die corners and the load
increases rapidly. The highest load is reached after the
workpiece fills completely the die cavity but before flash
starts to form.
� Zone IV: This zone covers up to 100% of the stroke. In
this zone flash is extruded through the flash land. In this
zone the load increases before the extrusion starts, then it
decreases when the material flows through the flash gap.
3.4. Determination of the optimum geometry of the tooling
The goals in the tooling optimization were to ®nd a
geometry that requires the smallest load to ®ll the die cavity
without causing defects. Load is an important factor in die
life.
As explained in Fig. 17, several simulations were per-
formed with different geometrical parameters (¯ash location
and thickness). The process parameters (punch speed, mate-
rial) were the same for all the simulations. The results of
these simulations are compared in Fig. 18.
The lowest loads are achieved with Geometry II. If the
¯ash gap is located in the same place as it was for Geometry I
and Ill, the load increases. There is a 27% difference
between the loads for Geometry I and II for a ¯ash thickness
of 0.8 mm (Fig. 18). This difference is 10% when the ¯ash
gap is 0.4 mm thick. The load difference is 22% between
Geometry II and Geometry III, with 0.8 mm of ¯ash thick-
ness. This difference drops to 6% when the ¯ash thickness
reaches 0.4 mm.
As in all hot forging operations, the load is a function of
the ¯ash thickness. When the ¯ash thickness decreases, the
load at the end of the forming process increases. In the ®rst
approach, the ¯ash thickness was estimated using the com-
Fig. 16. Parameters modified during the tooling optimization.
Table 3
Input data for the controlled flash forging simulations of the connecting
rod I-beam section
Parameter Value
Stroke 2.56 mm
Punch speed 20 mm/s
Material (characteristics taken from DEFORM database) Al 2618
Friction factor, m 0.2
Workpiece and die temperature 4008CFlash amount 5%
Fig. 17. Load-stroke curve for controlled flash forging.
V. Vazquez, T. Altan / Journal of Materials Processing Technology 98 (2000) 81±89 87
mon rules for ¯ash design [6]. These rules give a ¯ash
thickness of 1.6 mm. This thickness is the connecting rod
web thickness. The controlled ¯ash tooling allows a very
small amount of ¯ash. The biggest ¯ash thickness was set to
0.8 mm. This ¯ash thickness gives the lowest loads on the
tooling, as shown in Fig. 18.
The tooling with the geometry described above was
compared to a conventional closed-die tooling with the
same geometry. The amount of ¯ash for the billet in the
conventional closed-die forging was 18%. This is a common
amount of ¯ash for a conventional closed-die forging. The
controlled ¯ash forging gives a load 5% higher than the one
in closed-die forging (Fig. 18). If the billet volume has a
¯ash amount of 5%, the die cavity is not ®lled at the end of
the stroke for the conventional closed-die forging with ¯ash
(Fig. 19). For the ®nal geometry the ¯ash is located in the
middle of the tooling and the ¯ash thickness is 0.8 mm.
3.5. Non-isothermal forging simulation of the I-beam
section
Once the tooling geometry was de®ned, two non-isother-
mal simulations were performed. Since the process is a hot-
forging process, chilling the workpiece is an important
factor in the forging process. The simulation was performed
with the tooling Geometry II. This geometry gives the lowest
loads. The ¯ash gap thickness was set to 0.6 and 0.8 mm.
Only two simulations were performed because non-isother-
mal simulations are more time consuming than isothermal
ones. As expected, the computed loads increased about 13%.
This is mainly due to the workpiece chilling. These simula-
tions are compared in Fig. 20.
In the following section the results of the non-isothermal
simulation of the I-beam section, with the ®nal tooling
geometry are presented (Fig. 20). The parameters are the
same as those used in the isothermal simulations, except for
those speci®c to heat transfer (Table 4).
The temperature was uniformly distributed in all of the
parts at the beginning of the forming. The material ¯ow is
shown in Fig. 21. The die cavity is completely ®lled at the
end of the stroke with a ¯ash amount of 5%. This simulation
was completed without a gap between the punch and the
outer die. Thus, there is no ¯ash allowed in this area.
4. Conclusions and future work
In the case studies presented in this paper it has been
shown that physical and numerical modeling are helpful in
Fig. 18. Optimization on controlled flash forging tooling.
Fig. 19. Under filling on conventional closed-die forging with 5% of flash.
Fig. 20. Comparison isothermal and non-isothermal forgings.
Table 4
Parameters for the non-isothermal simulations [7]
Aluminum
2618
Tool steel
(AISI 301)
Thermal conductivity (W/m28C) 182 28
Heat capacity (�106 J/m38C) 2.84 3.56
Emissivity 0.15 0.15
Workpiece temperature at the beginning
of the forming (8C)
400
Dies temperature at the beginning of
the forming (8C)
200
Heat-transfer coefficient (kW/m2 K) 16 16
88 V. Vazquez, T. Altan / Journal of Materials Processing Technology 98 (2000) 81±89
the current design practices of forging processes due to the
following reasons:
� these techniques are generally cheaper than performing
tryout with actual dies and equipment,
� modifications to the tooling model (CAD design or soft
tooling) are cheaper and less time consuming than mod-
ifications of the actual production tooling and equipment,
� modeling provides more information about the process,
i.e.: load requirements and metal flow at different stages
of the process,
� for most applications the results may be obtained faster
from modeling than from actual tryouts,
� flashless forging results should be compared with results
obtained from forging with flash. This would help to
determine more clearly the advantages and disadvantages
of flashless forging,
� tool stress analysis of the tooling must be performed in
order to analyze the best way to achieve the longest tool-
life with the highest accuracy,
� flashless forging could result in significant material sav-
ings, however, a more strict control of the volume of the
preform is necessary,
� the new tooling concept presented allows a small amount
of flash (5%) compared to the conventional forging
processes that impose 20±40% of material waste.
� the tooling geometry was optimized using two-dimen-
sional simulations. The best results were obtained for a
tooling geometry with the flash gap in the middle of the
connecting rod and a flash thickness of 0.8 mm,
� the proposed tooling design allows to forge a near net
shape product as in flashless forging,
� unlike conventional and flashless forging tooling, the
proposed tooling will not be overloaded because the flash
is extruded radially without a normal load, i.e., the upper
die does not compress the flash.
References
[1] T. Altan, S.I. Oh, H. Gegel, Metal Forming- Fundamentals and
Applications, American Society of Metals (ASM), Cleveland, 1983.
[2] A. Barcellona, K. Long, T. Altan, Flashless Forging of a Connecting
Rod of an Aluminum Alloy and a Metal Matrix Composite (MMC)
Material, ERC/NSM-B-94-32, 1994.
[3] J. Mezger, K. Sweeney, T. Altan, Investigation of the 3D CODE:
Flashless Forging of a Connecting Rod, ERC/NSM-B-94-31, 1994.
[4] T. Takemasu, V. Vazquez, T. Altan, Investigation of metal flow and
preform optimization in flashless forging of a connecting rod, J.
Mater. Processing Technol. 59(1)(2) (1996) 95±105.
[5] K. Long, V. Vazquez, B. Painter, T. Altan, Flashless Forging of a
Metal Matrix Composite (MMC), ERC/NSM-B-95-31, The Ohio
State University, Columbus, OH, 1995.
[6] YT. Im, T. Altan, G. Shen, Investigation of the Effect of Flash
Dimensions and Billet Size in Closed Die Forging, ERC/NSM-B-88-
19, The Ohio State University, Columbus, OH, 1988.
[7] P. Burte, S. Semiatin, T. Altan, Measurement and Analysis of Heat
Transfer and Friction During Hot Forming (Final Report), ERC/
NSM-B-89-20, The Ohio State University, Columbus, OH, 1989.
Fig. 21. Flow pattern for non-isothermal forging, Geometry I, flash
thickness 0.8 mm.
V. Vazquez, T. Altan / Journal of Materials Processing Technology 98 (2000) 81±89 89