Some researches upon the tool-piece contact geometry in the rolling process.
Lupescu, Octavian ; Popa, Ramona ; Popa, Ionut 等
1. PROBLEM STATEMENT
The superficial cold plastic deformation (SPD) is a mechanical
treatment method of the metallic materials that allows us to obtain the
mechanic characteristics improvement (Lupescu et al., 2004), the
expensive materials changeover with any other cheaper, hardened using
SPD process, as well as the thermo and thermo-chemical secondary
treatments changeover because of their amount prices.
This technical paper shows also a surface geometry determination of
the deformation focus, in case of the rolling hardening with disk rolls
(Lupescu et al., 2001).
2. APPLICATION AREA
The researches objective was to determine the tool-piece surface
contact projection on the tangent plan, in their initial contact point.
The literature (Lupescu, 1999) shows that process is able to be
applied to cylindrical pieces, especially to big diameters (>100 mm),
for individual series and also mass production series. The degree
hardness resulted on superficial layer (until 1 -1, 5 mm) exceed in many
cases with 10% (Lupescu & Baciu, 2002) the obtained results of the
thermo-chemical treatments.
3. METHOD USED
First of all, there were established the curved radius taking into
account the elastic deformation which affect the rolls. For the second
step, the deformation focus surface results taking into consideration
the plastic and elastic deformations aboard the working piece (figure
1).
Using the general relation to establish a surface curved radius
elastic deformed (Lupescu et al., 2005):
1/[R.sup.*.sub.1,2] = 1/2 (1/[R.sub.I,1(2)] - 1/[R.sub.II,1(2)] (1)
the authors suggest for the curved radius of the roll attack
surface in the case of his elastic deformation, the following relations:
1/[R.sup.*.sub.1] = 1/2 (1/[R.sub.I,1] - 1/[R.sub.II,1]) = 1/2 x
1/[R.sub.I,1]; [R.sup.*.sub.1] = 2[R.sub.II] (2)
1/[R.sup.*.sub.2] = 1/2 (1/[R.sub.I,2] - 1/[R.sub.II,2]) = 1/2 x
1/[R.sub.I,1]; [R.sup.*.sub.2] = 2[R.sub.12][R.sub.22]/[R.sub.22] -
[R.sub.12] (3)
[FIGURE 1 OMITTED]
Working in a Cartesian system OXYZ because of the elastic roll
deformations under the F force action, his initial radius [R.sub.11] and
[R.sub.12] belonging to the principal two plans will be modified to
[R.sup.*.sub.1] and [R.sup.*.sub.2] with their centers displacement from
[O.sub.1] to [O.sup.*.sub.1] and from [O.sub.2] to [O.sup.*.sub.2].
Using the next notation, the total contact deformation will be:
[bar.CD] = [delta] = [[delta].sub.el] + [[delta].sub.pl], thus: (4)
[[DELTA].sup.*] = [R.sup.*.sub.2] + [R.sub.22] - [delta], so: (5)
[O.sup.*.sub.1]A = [square root of [R.sup.*2.sub.1] -
[[bar.AB].sup.2]] = [square root of [R.sup.*2.sub.1] - [x.sup.2]], and:
(6)
[O.sup.*.sub.1] [O.sup.*.sub.2] = [R.sup.*.sub.2] -
[R.sup.*.sub.1], and: (7)
[[bar.BB].sup.*] = [([R.sup.*.sub.2] - [R.sup.*.sub.1]) + ([square
root of [R.sup.*2.sub.1] - [x.sup.2]])] (8)
The deformation surface equation, belonging to the
[O.sup.*.sub.2][X.sup.*.sub.2][Y.sup.*.sub.2][Z.sup.*.sub.2] system is:
[y.sup.*2.sub.2] + [z.sup.*2.sub.2] - [[bar.BB].sup.*2] = 0 and so:
(9)
[y.sup.2.sub.2] + [(z - [[DELTA].sup.*]).sup.2] -
[[([R.sup.*.sub.2] - [R.sup.*.sub.1]) + [square root of [R.sup.*2.sub.1]
- [x.sup.2]]].sup.2] = 0 (10)
In these conditions, the contact surface curve can be determined
with the system equations:
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (11)
The outline intersection of two bodies (tool-piece) projected on
the tangent plan in the initial contact point is an ellipse whose
expression was obtained from (11):
[y.sup.2] + [[R.sup.2.sub.22] + [[DELTA].sup.2] -
[[([R.sup.*.sub.2] - [R.sup.*.sub.1]) + [square root of [R.sup.*2.sub.1]
- [x.sup.2]]].sup.2]]/2[[DELTA].sup.*]] - [R.sup.2.sub.22] = 0 (12)
The equation of the real contact surface in the elastic-plastic
deformation process was solved using the overlap effects principle.
4. RESULTS
Thus, on the first step, it was admitted only the static contact of
the elements. The ellipse from the tangent plan results like projection
of the determination focus surface (figure 2) with (a) and (b) semi-axis
established by (12); the small semi-axis (b) is the y value from this
equation, when x = 0 and the big one (a) is the limit value of x when
the above equation ensure the real values for y.
On the second step it was simulated the axis movement of the
contact ellipse along the longitudinal speed direction of the deforming
roll.
On the left side, the roll came into contact with the working
piece, on the existing surface from the last step. On the right side the
roll remain in contact with the piece on a reduce surface, because of
his plastic deformation.
Thus, on the right side, the intersection outline is an elliptic contour having ([a.sub.I]) semi-axis, taking into account the elastic
contact only. The semi-axis (b) is unchangeable. So:
[a.sub.I] = [a.sup.*] [cube root of 3F/E [summation] [zeta]],
where: [a.sup.*] = [[2k[xi](e)/[pi]].sup.1/3] (13)
On the third step, one simulates the tool rotation either, along
side OY axis. The new surface contour is represented in figure 3. In
this case also, behind the roll, it remains a reduced contact surface,
resulted only due to the plastic piece deformation.
Thus, during the rolling process, the real contact between
tool-piece is produced on a contact surface having the following curved
sectors:
* AB, remained from the initial unmodified ellipse, whose equation
is done after relation 12;
* BC, ellipse arc which has a semi-axis (b) and the other semi-axis
([a.sub.I]) resulting from relation 13. The analytically expression of
these outline is:
[(x/[a.sub.I]).sup.2] + [(y/b).sup.2] - 1 = 0 (14)
* CD, ellipse arc having ([a.sub.I]) and respectively ([b.sub.II])
semi-axis, calculated from the elastic pure contact conditions:
[b.sub.II] = b [cube root of 3F/E [summation] [rho]], where:
[b.sup.*] = [[2[xi](e)/[pi]k].sup.1/3] (15)
[FIGURE 2 OMITTED]
[FIGURE 3 OMITTED]
The contact expression outline on this sector becomes:
[(x/[a.sub.I]).sup.2] + [(y/[b.sub.II]).sup.2] - 1 = 0 (16)
* DA, ellipse arc with (a) semi-axis and the other equal with
([b.sub.II]), when the analytically contour expression becomes:
[(x/[a.sub.II]).sup.2] + [(y/[b.sub.II]).sup.2] - 1 = 0 (17)
In these conditions, the mathematic expression became:
z = [[DELTA].sup.*] - [square root of [[R.sup.*.sub.2] -
[R.sup.*.sub.1]] + [square root of [R.sup.*2.sub.1] - [x.sup.2] -
[y.sup.2]]] (18)
with X and Y values being throughout the outline delimited by the
ellipse arcs AB, BC, CD and DA, anterior defined.
5. FURTHER RESEARCHES
The determined focus surface afterwards will allow: the contact
surface pressure establishment, the slides speeds between the couple
elements, the power friction consumed during the process and friction
parameters establishment using the lubricant film calculus.
6. REFERENCES
Lupescu, O., (1999), Surfaces polishing through plastic deformation
and steels cold hardening proces (Netezirea suprafetelor prin deformare
plastica si durificare la rece a otelurilor), Junimea, ISBN 973-37-0471-7, Iasi
Lupescu, O., et al., (2001), The device choosing for rolling the
exterior cylindrical surface using the utilities theory, Proceedings of
Modern Techniques, Quality, Reorganization, vol. 1, pg. 229-232,
Chisinau
Lupescu, O., Baciu, M., (2002), The characterization of mechanical
treatment at SPD at cold through rolling as a tribological process,
Proceedings of Meridian Engineering, 12 (3), pg. 29-32, Chisinau
Lupescu, O., et al., (2004), Structural modification of the Ol 25
Steel in the Cold SPD Process Through Rolling, Academic Journal of
Manufacturing Engineering, 2(4), pg.43-47, Timisoara
Lupescu, O., et al., (2005), About the establishment of surface
geometry for the SPD process by rolling, Proceedings of
Machine--Building and Technosphere of the XXI Century, Tom. 4, 12-17
September., 255-260, Sevastopol