Aggressive turning for enhanced productivity.
Urbicain, Gorka ; Fernandez, Asier ; Olvera, David 等
1. INTRODUCTION
Minimizing production time is a key objective in every machining
process. Due to the high cost of the NC integrated into the machining
centre, a productive approach to the process is required in order to
obtain the payback in a reasonable time. This need of optimizing the
cutting values is even more important in rough machining where the high
chip evacuation rate increases the opportunities for time and cost
savings (Meng et al., 2000). Concerning stability prediction models,
Tlusty and Polacek (Tlusty & Polacek), used an approximate solution
reducing the dynamics problem into a 1D case. Although this can be valid
for plunge turning or straight turning where the inclination angle and
the nose radius are neglected, it may not be accurate for
multidimensional cutting processes or dynamics. This paper presents two
different approaches to optimize productivity in medium turning. The
first approach predicts the stable cutting parameters using the
frequency-domain method based on the model from Altintas and Budak
(Altintas & Budak, 1995) which is then contrasted with validation
tests. The second one is based on a relatively new alternative,
turn-milling, which allows for high feed speeds and increased depths of
cut. This process is preliminary investigated by means of tool life
testing.
2. STABILITY PREDICTION IN TURNING
The following model is based on the frequency-domain method
proposed by Budak and Ozlu (Budak & Ozlu, 2007) which discretizes
the tool radius to enhance the accuracy of the stability plot. In this
case, unlike the previous one, the method is applied to different
cutting depths with global coefficients which account for the total
cutting energy put into play.
2.1 Stability model
The most significant assumptions of the model are:
* Single DOF in radial direction
* Flexible workpiece-rigid tool
* Cutting coefficients dependents of the depth of cut
* Side cutting edge angles defined from the depth of cut average of
the corresponding element
The force model uses a simple linear dependency between the chip
thickness and the cutting force. Thus, the effect of the friction is
absorbed by the pure cutting. Fig. 1 shows the model scheme associated
with a simple turning operation. The steadystate force in radial
direction is expressed as shown in Eq. 1:
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (1)
[FIGURE 1 OMITTED]
For dynamic analysis, only the variable force is considered:
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (2)
The vibration vector, difference between the actual and the
previous periods, can be expressed using the transfer function matrix
[G.sub.xx] ([[omega].sub.c]) in X direction:
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (3)
Introducing Eq. 3 in the dynamic force equation (Eq. 2), it results
the final expression for the study of the system stability:
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (4)
This is an eigenvalue problem which solutions represent the
stability boundary limits. The proposed method uses global cutting
coefficients obtained from cutting tests at different depths of cut:
from 0.5 to 2 mm with variable cutting speeds from 200 to 600 m/min
(f=0.4 mm/rev). Tab. 1. shows the specific forces for two different
depths of cut obtained as continuous functions of the cutting speed by
means of a second degree polynomial.
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII]
2.2 Experimental validation
The operations were carried out in a CMZ [T.SUB.C]25BTY turning
centre with a FANUC 31iT HVi numeric control. A test part made of AISI 1045 (D = 150 mm and L = 150 mm) was machined with a round carbide
insert (RCMT 08 03 MO 4225 by Sandvik) for medium turning. Tool holder
is placed with the minimum length to sustain the rigid tool assumption.
During the characterization of the inserts as well as in chatter tests,
the cutting forces were measured using a 9257B Kistler dynamometer. The
signals are then amplified towards an OROS multi-channel analyzer and
processed with Matlab9. The modal parameters of the workpiece were
proved to remain practically constant during each chatter test but
variable from one test to another. Tab. 2. shows the main values used
for two of the simulations (ap=1 and 1.5 mm). The FRF values were
obtained through impact hammer tests before each chatter test. Here, the
discretization of the tool radius has been achieved with 4 elements
(n=4) with 0.5 mm width (ap from 0 to 2 mm). Each depth of cut
considered corresponds with a global cutting coefficient averaged in the
range of study (Vc from 200 to 600 m/min). One important feature when
using tool discretization models, even more for round inserts due to a
nonlinear geometry of the edge, lies on the estimation of the effective
side cutting edge angle acting at each depth of cut studied. In this
case, the side cutting edge angle is defined at each element's mean
depth of cut (see Eq. 5.):
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (5)
Fig. 2. and Fig. 3. represent the stability lobe diagrams and their
ma[T.sub.c]h with the experimental tests conducted for ap=1 and ap = 1.5
mm.
[FIGURE 2 OMITTED]
[FIGURE 3 OMITTED]
3. A NEW ALTERNATIVE: TURN-MILLING
3.1 Introduction to turn-milling
The kinematics of the turn-milling process is based on a
simultaneous rotation of the pair tool-workpiece, appearing in
multi-task machines of 4 to 5 axes. This technique can be categorized as
coaxial or orthogonal depending on the spatial position of the rotation
axes. It is called coaxial when the axis of rotation of the tool and the
piece are parallel to each other. This option is suitable for both
external and internal machining. On the other hand, it is called
orthogonal when the axis of rotation of the tool is perpendicular to the
piece, which is only applicable for external machining. The application
of this technique offers great opportunities increasing productivity
compared with conventional turning or milling operations (Choudhury
& Bajpai, 2005) due to its flexibility. This aspect eliminates
transition times and reduces the number of tools. From the point of view
of the determination of the optimal cutting conditions, the estimation
of the tool life and cutting forces with an acceptable degree of
accuracy is essential due to their strong effect on the main
restrictions imposed to the part.
3.2 Tool life analysis
The experiment was anew conducted in the CMZ turning machine with
four degrees of freedom using the orthogonal strategy. The test part is
a cylinder of AISI 1045, with initial diameter D=152 mm and L=160 mm of
working length. Tool wear is studied in carbide inserts with four
cutting edges (RCKT M0) with D=50 mm. In order to control the wear of
the inserts during the cutting tests, systematic measurements were
carried at different machining lengths (each 480 mm). The values
obtained for the four cutters were averaged to plot the wear curve shown
in Fig. 5.
[FIGURE 4 OMITTED]
4. CONCLUSIONS
When it comes to part manufacturing and production, it is a key
issue to define optimized cutting conditions before their introduction
to the process chain. In this sense, the study proposes, on one hand, an
analytical approach for the stability prediction with successful degree
of matching between simulations and experimental results what allows to
fix stronger cutting conditions. Future research will focus on one hand
on exploring the benefits of such a model not only for the assumption of
flexible workpiece but for flexible tool as well as the possibility of
using new mathematical algorithms which allow to introduce variable
coefficients (with the depth of cut and with the cutting speed) as well
as more reliable side cutting edge angles. On the other hand,
turn-milling is preliminary studied by means of the evolution of the
tool wear resulting in controlled values with the simultaneous aim of
stronger conditions but safeguarding the life of the tool. Future plans
include a force model to predict the cutting forces and a surface
roughness prediction model.
5. REFERENCES
Altintas, Y. & Budak, E. (1995). Analytical prediction of
stability lobes in milling, Annals of the CIRP 44 (1) 357362
Budak, E. & Ozlu, E. (2007). Analytical Modeling of Chatter
Stability in Turning and Boring Operations: A Multi-Dimensional
Approach, CIRP Annals-Manuf. Tech. 56 (1) 401-404
Choudhury, S.K. & Bajpai, J.B. (2005). Investigation in
orthogonal turn-milling towards better surface finish, Jour. Mat. Proc.
Tech. 170 (3) 487-493
Meng, Q.; Arsecularatne, J.A. & Mathew, P. (2000). Calculation
of optimum cutting conditions for turning operations using a machining
theory, Int. Jour. Mach. Tools & Man. 40 1709-1733
Tlusty, J. & Polacek, M. (1963) The Stability of Machine Tools
Against Self Excited Vibrations in Machining, Proc. of the Int. Research
in Production Engineering Conference, Pittsburgh, PA, ASME, New York,
pp. 465-474
Tab. 1. Specific cutting force: polynomial approach
Ap [mm] Key[N/m[m.sup.2]] (Vc [m/min])
1 -0.00207xV[c.sup.2] + 2.061 x Vc + 885.75
1.5 0.00305 x V[c.sup.2] - 1.3880 x Vc + 1150.77
Tab. 2. Modal parameters, global specific cutting forces and
side cutting edge angles
FRF modal parameters
ap Key (avg.) [kappa]
[mm] f [Hz] [xi] k [N/m] [N/mm2] [[degrees]]
1.00 160.3 9.80e-3 5.88e+7 1553.6 28.96
1.50 139.7 4.22e-2 2.98e+7 1282.2 35.66