Upload
wang-guangchun
View
214
Download
0
Embed Size (px)
Citation preview
A three-dimensional rigid±plastic FEM analysis of rotary forgingdeformation of a ring workpiece
Wang Guangchun*, Zhao Guoqun
Mold and Die Engineering Center, Shandong University of Technology, Jinan, Shandong 250061, China
Received 12 April 1998
Abstract
The deformation of a ring workpiece by the rotary forging process is analyzed using a three-dimensional rigid±plastic ®nite element
method. Velocity ®elds and stress±strain ®elds of the ring workpiece in the rotary forging deformation are obtained. The new metal ¯ow
demarcation model obtained in this paper is different from that ever provided before. The deformation mechanism of the rotary forging of
the ring workpiece is revealed thoroughly. # 1999 Elsevier Science S.A. All rights reserved.
Keywords: Ring workpiece; Rotary forging; Deformation analysis; FEM
1. Introduction
Rotary forging is a new rotaform process which deforms
only a small portion of a workpiece at a time using a conical
rocking die whose axis is tilted at an angle with respect to the
axis of the other die or the workpiece. To date, this technol-
ogy has been applied widely in practice, but many problems
involved in this technology have not yet been solved. The
majority of current researchers have not exploited the the-
oretical aspect. Most of their work still remains experimen-
tal due to the eccentric load of the process and the
complicated contact contour and shape between the conical
upper die and the workpiece. Especially for a ring work-
piece, there still exist many unsolvable problems in manu-
facturing. The related technical problems have to be solved
by the trial-and-error method. The ®nite element analysis
method has been proved a good method, which can obtain
more detailed information in analyzing metal working and
applied for almost types of metal forming processes. How-
ever, so far, from the present survey of the literature, this
method has hardly been used to analyze the rotary forging
process.
2. Fundamental principle of the rigid±plastic FEM
The rigid±plastic FEM solution equations usually satisfy:
the equilibrium equation; the geometrical equation; volume
constancy; the assumption of not considering volume force;
neglecting the elastic deformation of the material; and the
material con®rming to the Mises Yield criterion. Using the
penalty function method to handle the condition of volume
constancy, the energy function is expressed as follows:
� �Z� _�" dV � �
2
Z� _"V�2 dV ÿ
ZST
Fiui dS; (1)
where �� is the equivalent stress, _�" the equivalent strain rate,
� the penalty factor, _"V the volume strain rate, V the volume
of the deformating body, Fi the external force, ui the velocity
at the surface ST and ST is the area of the surface acted upon
by the external force.
3. Finite-element model of the rotary forging processof a ring workpiece
In rotary forging, the relative motion between the work-
piece and the conical upper die is a spiral penetration. The
contact surface is a portion of an Archimedes spiral surface,
as shown in Fig. 1. The eight-node hexahedron isopara-*Corresponding author. Tel.: +86-0531-6041359; fax: +86-0531-2953-
623.
Journal of Materials Processing Technology 95 (1999) 112±115
0924-0136/99/$ ± see front matter # 1999 Elsevier Science S.A. All rights reserved.
PII: S 0 9 2 4 - 0 1 3 6 ( 9 9 ) 0 0 2 6 8 - X
metric element was used and the workpiece was divided into
900 elements and 1200 nodes, as shown in Fig. 2.
The contour and shape of the contact zone can be calcu-
lated according to the rotary forging parameters and the
geometrical dimensions of the workpiece. The zone sur-
rounded by points A, B, C and D can be adjusted according
to the actual situation under analysis. All nodes at the bottom
surface of the workpiece are ®xed in both the axial and
tangential directions. The velocity boundary condition of the
contact surface is exerted automatically by the normal
direction cosine of the contact surface according to the
rotary forging parameters. The frictional model proposed
by Chen and Kobayashi is used here [1]. The other deforma-
tion conditions are: rocking angle �38; feed S�1.34 mm/
rev; friction factor m�0.2; outside diameter of the work-
piece D0�70 mm; inside diameter of the workpiece
d0�40 mm; height of the workpiece H0�40 mm.
4. Metal flow patterns of a ring workpiece in rotaryforging
On the basis of the principle of rigid±plastic FEM and
according to the established mechanical model, a set of
three-dimensional FEM programs was developed and used
to analyze the rotary forging deformation of the ring work-
piece [2,3]. Fig. 3 shows the metal ¯ow ®elds of the axial
section and the cross section, respectively. The metal in the
contact layer ¯ows mainly along the radial direction. Fig. 4
gives a new metal ¯ow demarcation pattern in the contact
surface layer obtained by FEM analysis results. The metal
near to the exit ¯ows along the same tangential direction as
that of the rotation of the upper die whilst the metal at the
entrance ¯ows along the reverse direction of the rotation the
upper die. R� indicates that the metal ¯ows outside along the
radial direction, and Rÿ inside along the radial direction. T�
indicates that the metal ¯ows along the tangential direction,
which is the same as that of rotation of the upper die. Tÿ is
the reverse direction of rotation of the upper die. From
Fig. 3(b), it can be seen clearly that the metal at the contact
surface layer ¯ows both inside and outside along the radial
direction when it is compressed in the axial direction. The
metal ¯ow demarcation line locates near the inside wall of
the ring workpiece.
The metal ¯ow laws at the contact surface layer of a ring
workpiece can be stated as follows. The metal is compressed
in the axial direction and ¯ows mainly along the radial and
tangential directions. Along the radial direction the metal
¯ows from the demarcation line to either the inside or the
outside. The demarcation line is near to the interior of the
inside wall of the ring workpiece because the resistance to
metal ¯ows to the inside is greater than that to the outside. At
the same time, the metal located at the entrance and the
exit ¯ows to the center of the contact zone along the
tangential direction due to the strong restraint by the non-
contact zone.
Fig. 1. Geometrical description of the shape of a ring workpiece in rotary
forging.
Fig. 2. Discretization meshes of a ring workpiece in rotary forging.
Fig. 3. Velocity fields of a ring workpiece at the contact layer in rotary
forging: (a) cross section; (b) axial section.
Fig. 4. New metal flow demarcation pattern in the contact surface layer in
the rotary forging of a ring workpiece.
W. Guangchun, Z. Guoqun / Journal of Materials Processing Technology 95 (1999) 112±115 113
5. Deformation mechanism of the ring workpiece inrotary forging
From the whole process of the deformation, rotary forging
process of the ring workpiece is somewhat similar to upset-
ting, but is rather different from the upsetting because both
the forging load and the geometric shape of the contact zone
are non-symmetrical. From the view of loading conditions, it
is also similar to the rolling process, but there is also quite a
difference from the rolling process because of the differ-
ences of the load and boundary conditions, the load situation
and boundary conditions of the rotary forging process all
being very complicated. Fig. 5 shows the strain rate dis-
tributions of the ring workpiece in the rotary forging, whilst
Fig. 6 shows the stress distributions of the ring workpiece.
From Fig. 5, it can be seen that the workpiece is compressed
Fig. 5. Strain-rate distributions in the surface of the ring workpiece in rotary forging: (a) _"r ; (b) _"�; (c) _"z; (d) _�".
Fig. 6. Stress distributions in the surface of the ring workpiece in the rotary forging: (a) �r (MPa); (b) �� (MPa); �z (MPa); ���MPa�.
114 W. Guangchun, Z. Guoqun / Journal of Materials Processing Technology 95 (1999) 112±115
in the axial direction and elongated along the radial direc-
tion. The deformation zone expands to a certain extent at the
contact surface layer and shrinks gradually downwards
along the height. The shape of the deformation zone is like
that of a funnel. From Fig. 6, it can be seen that the contact
deformation zone suffers three-dimensional negative stress,
where the absolute values of the axial stress and the equiva-
lent stress decrease gradually with height. From the above
analysis, the following deformation mechanism of the rotary
forging process of the ring workpiece is obtained.
(1) Because the workpiece is loaded partly and eccen-
trically by the conical upper die along the axial direction, the
metal at the local contact layer yields ®rstly and then
deforms.
(2) The absolute value of the axial stress becomes smaller
as the area of the loaded zone becomes larger downwards.
The deformation zone concentrates mainly on the upper part
of the ring workpiece and the area of the deformation zone
decreases gradually along the axial direction and shows a
funnel shape.
(3) At the contact surface layer, the metal is compressed in
the axial direction and shows strong tensile deformation in
the radial direction because of the strong tangential restraint
by the non-contact zone. This results in the inside diameter
shrinking and the outside diameter increasing.
(4) That the contact surface is loaded partly by the conical
upper die results in the strong tangential deformation along
the same direction as the rotation of the upper die. With the
ring workpiece being loaded intermittently and formed
successively, the deformation is accumulated gradually until
the required ring shape is accomplished ®nally.
6. Conclusions
(1) The mechanical model of the rotary forging process of
a ring workpiece with three-dimensional rigid±plastic ®nite
element method presented in this paper is in accordance with
the actual deformation conditions.
(2) The deformation in the rotary forging of a ring
workpiece results mainly from the yielding of the metal
at the local layer zone. Because the ring workpiece is loaded
locally and eccentrically by the conical upper die in rotary
forging, the metal at the local contact surface layer zone
yields and deforms ®rstly. The metal here is compressed in
the axial direction and elongated along the radial and
tangential directions. The absolute value of the axial stress
decreases gradually downwards and the deformed zone is
concentrated mainly on a small portion of the upper part of
the ring workpiece.
(3) Due to the restraint of the non-contact zone along the
tangential direction, the metal at the contact surface layer
¯ows mainly from the middle deformation zone to either
inside or outside along the radial direction. The demarcation
line is near to the interior of the inside wall of the ring
workpiece. Along the tangential direction, the metal at the
contact surface layer ¯ows from the entrance and exit to the
center because of the strong restraint from the non-contact
zone.
(4) That the contact surface is loaded partly by the conical
upper die results in the strong tangential deformation along
the same direction as of the rotation of the upper die.
Acknowledgements
This research work has been supported by the Shandong
Province Outstanding Young Scientists Grant 97235510
and the Shandong Province Nature Science Fund
Y98F08089.
References
[1] C.C. Chen, S. Kobayashi, Rigid plastic finite element analysis of ring
compression, Application of numerical methods to forming process,
ASME AMD 28 (1978) 107.
[2] G. Wang, A 3D rigid±plastic FEM analysis of rotary forging
deformation of ring workpieces, Ph.D. Dissertation, HIT, April
1996.
[3] G. Wang et al., Methods of dealing with some problems in analyzing
rotary forging with the FEM and initial application to a ring
workpiece, J. Mat. Proc. Tech. 71 (1997) 299±304.
W. Guangchun, Z. Guoqun / Journal of Materials Processing Technology 95 (1999) 112±115 115