Experimental investigation of vibrational drilling/Vibracinio grezimo eksperimentinis tyrimas.
Ubartas, M. ; Ostasevicius, V. ; Samper, S. 等
1.
2. Introduction
Higher productivity and better surface quality are the
prerequisites for current machining industry to be more competitive
since modern manufacturing processes require shorter production time and
higher precision components. Field of metal machining is closely linked
to different industrial sectors including automotive, construction,
aerospace, transport, medical, mechanical engineering, etc. Material
treatment using cutting is still one of the predominant technological
processes for manufacturing high-precision and complex components [1,
2]. Cutting force and speed, feed-rate, temperature in the contact zone
are those key variables that significantly influence surface quality and
tool life [3, 4]. Control of these parameters affects the entire
manufacturing process. Constant pursuit for more effective cutting
methods revealed that machining quality can be improved if the tool is
assisted with ultrasonic frequency vibrations, i.e. small-amplitude
(typically 2-20 |am) and high-frequency (typically up to 20 kHz)
displacement is superimposed onto the continuous cutting motion of the
tool. During the resulting vibration(al) cutting process [5] the tool
periodically looses contact with the chip or leaves the workpiece
entirely. As a result, machining forces, friction and temperature in the
cutting zone decrease, thinner chips are generated, formation of
micro-cracks on the cutting edge and workpiece surface is impeded as
opposed to the case of conventional machining. This, in turn, leads to
enhanced cutting stability, surface finish and form accuracy as well as
extended tool life and near-zero burr compared to conventional processes
[6]. Surface quality can be improved to such an extent that it may
enable complete turning, milling, boring and other cutting processes;
(b) according to estimations the waste constitutes about 10% of all the
material produced by machining industry [7].
In works [8, 9] it was reported that vibrational turning and
milling processes are more effective with respect to traditional methods
and the resulting surface quality of the workpiece is markedly improved.
L.B. Zhang in his work [10] concluded that at the same cutting
conditions, the thrust and the torque during vibrational drilling are
reduced by 20-30% when compared to conventional process. V. Ostasevicius
et al. in their recent research work [1] proposed a feasible solution
for improvement of surface quality of the workpiece in vibrational
turning by virtue of advantageous application of the specific higher
vibration mode of the cutting tool.
Vibrational cutting technology has already matured to an extent
which is sufficient for several limited industrial applications.
However, the understanding of fundamental mechanisms participating in
the associated machining processes is still incomplete. Therefore,
vibrational cutting still remains a topic of active scientific research
since substantial efforts are required in order to develop reliable
computational models that would allow optimization of the processes for
specific materials and operating conditions.
Promising results obtained during research of vibrational turning
and milling processes [1, 8, 9] encouraged the authors of this paper to
focus on drilling since it is one of the most common machining processes
due to the need for component assembly in mechanical structures.
This paper presents results of experimental investigation of
vibrational drilling, which was carried out by using a prototype of tool
holder that was developed at Kaunas University of Technology [11].
Reported research results indicate that vibrational drilling process is
characterized by reduced axial cutting force and torque in comparison to
the traditional drilling. It is demonstrated that control of tool
vibration mode through application of appropriate excitation frequency
enables to maximize the degree of reduction of surface roughness as well
as axial cutting force and torque.
3. Experimental setup
Vibrational drilling experiments were carried out at the Laboratory
of Systems and Materials for Mechatronics (SYMME) of the University of
Savoie (France) by using CNC milling machine YANG SMV-600 with work
pieces made of steel C48. The experiments were performed with the
developed vibrational drilling tool (Fig. 1) that employs piezoceramic
rings implemented in the tool holder for generating ultrasonic
vibrations of the drill cutting edge 10 [11]. A piezoelectric transducer
is the source of mechanical oscillations, which transforms the
electrical power received from the power supply. The power is supplied
to the drill device through collector rings 4. Ultrasonic power supply
generates up to 200 W with sinusoidal waveform. A stack of two
piezoelectric rings 8 converts the electrical power into mechanical
vibrations. A concentrator 9 is fitted onto the end of the transducer,
which leads to intensification of drill-tip vibration amplitude that may
reach up to 20 | m. The vibrational drilling tool is designed to operate
in the resonance mode.
Vibrational drilling experiments were conducted by exciting the
tool with the two first resonant frequencies. They were determined by
means of tool frequency response measurements that were performed by
using experimental setup presented in Fig. 2. Vibrations were registered
through acceleration sensor KD-91 (k = 0.5 mV/(m/[s.sup.2])), which was
fixed on the drill-tip (position A in Fig. 2). The obtained signal was
converted and transmitted to the computer via analog-digital converter
(digital oscilloscope PICO 3424). PicoScope software was used for
processing and visualization of results (Fig. 3).
[FIGURE 1 OMITTED]
4-component dynamometer platform KISTLER 9272 was used for
measuring the magnitudes of axial cutting force and torque that are
generated during the drilling process (Fig. 4). Cylindrical workpieces
were mounted on the clamping device of the dynamometer, while the latter
was installed on the desk (Fig. 5). The energy from the high-frequency
generator (Fig. 6) was transmitted to the drill. Cutting force and
torque during drilling operations were measured, registered, the signal
was transmitted to the computer, where a special software developed by
CTDEC (Centre Technique de l'Industrie du Decolletage (France)) was
used for signal analysis.
[FIGURE 2 OMITTED]
4. Testing procedure
Measured amplitude-frequency characteristic (Fig. 3) indicates two
main resonances at the excitation frequencies of 12 kHz and 16.6 kHz for
the twist drill of [empty set]10 mm. These frequencies were applied for
tool excitation during vibrational drilling experiments (Fig. 4), which
were carried out by using the following regimes: drilling depth - 15 mm,
feed-rate - 0,2-0,25 mm/r, drilling speed 600-900 r/min. Analogous
experiments were repeated for the case of conventional drilling process.
For each different cutting condition two drilling holes and cutting
force/ torque measurements were performed. For each feed and cutting
speed ratings three force/torque measurements were performed. Obtained
experimental results are provided in Figs. 7-8.
[FIGURE 3 OMITTED]
[FIGURE 4 OMITTED]
[FIGURE 5 OMITTED]
[FIGURE 6 OMITTED]
5. Analysis of results
Variation of axial cutting force and torque presented in Figs. 7
and 8 respectively demonstrate the comparison between conventional
drilling and the vibrational drilling at the first resonant frequency of
12 kHz in the case of three different feed-rates. These characteristics
reveal insignificant difference between magnitudes of axial cutting
force and torque for conventional and vibrational drilling processes.
Variation of axial cutting force and torque presented in Figs. 9
and 10 respectively provide the comparison between conventional drilling
and vibrational drilling at the second resonant frequency of 16.6 kHz.
Obvious difference in force and torque magnitudes is observed in this
case. Compared with conventional drilling, the cutting force during
vibrational drilling decreases by 12-46%. Meanwhile torque measurements
at the second resonant frequency indicate reduction of 13-20%. The most
pronounced difference between force and torque magnitudes in
conventional and vibrational drilling is detected at the largest
feed-rate of 0.25 mm/r, meanwhile the least pronounced difference is
observed at the smallest feed-rate of 0.2 mm/r. These measurement
results for axial cutting force and torque unambiguously demonstrate the
importance of tool vibration mode control in vibrational drilling
process, i.e. positive effect of superimposed high-frequency vibrations
is intensified when higher vibration mode is excited in the tool at a
larger driving frequency of the piezoelectric transducer.
[FIGURE 7 OMITTED]
[FIGURE 8 OMITTED]
[FIGURE 9 OMITTED]
After drilling experiments the machined cylindrical workpieces were
subjected to roughness measurements by using roughness tester TIME
TR2001. Workpiece roughness [R.sub.a], obtained when drilling at
excitation frequency of 12 kHz, is lower approximately by 10% in
comparison to the case of conventional drilling (reduction of [R.sub.a]
from 1.7 um to 1.45 um). After vibrational drilling at the second
resonant frequency of 16.6 kHz the workpiece surface roughness decreased
by down to 25% (from 1.7 um to 1.2-0.98 [micro]m) with respect to
conventional drilling. It is obvious that tool excitation at the first
resonant frequency insignificantly influences workpiece quality.
Transverse vibrations are damped at the contact point between the tool
and the workpiece - the longitudinal vibration amplitude is not
sufficiently high in this case. At the excitation frequency of 16.6 kHz
torsional and longitudinal vibration amplitudes become maximum and the
influence on the workpiece surface quality is much more pronounced.
Thus, these experimental findings reveal that in terms of surface
roughness the positive effect of vibrational drilling is also enhanced
when the tool is excited with higher vibration mode.
[FIGURE 10 OMITTED]
Drill-tip vibration (time response) measurements were also
performed in order to gain a deeper insight into dynamic tool behavior,
which could explain the results obtained during drilling experiments.
Tool vibrations were measured by means of two acceleration sensors KD-91
(k=0.5 mV/(m/[s.sup.2])). For these measurements a particular scheme
(Fig. 2, position A) was used: two single-axis acceleration sensors were
fixed on the drill-tip (Fig. 11). The registered signals were converted
and transmitted to the computer via PICO 3424 digital oscilloscope,
where PicoScope software was used for analysis of results.
[FIGURE 11 OMITTED]
[FIGURE 12 OMITTED]
For the case of tool excitation at the first resonant frequency (12
kHz) signal curves are almost concurrent, which indicates that the tool
undergoes both longitudinal and transverse vibrations (Fig. 12). During
tool excitation at the second resonant frequency (16.6 kHz) signal
curves are moving in different directions at the same time, thereby
revealing that two single-axis sensors register torsional vibrations
(Fig. 13). Excitation at 16.6 kHz induces both torsional and
longitudinal vibrations in the tool.
Another series of time response measurements were performed with
the purpose to evaluate how tool holder generates and transfers
vibrations to the drill. In this case the second acceleration sensor was
fixed at the end of the concentrator (Fig. 2, position B).
Measurement results are provided in Figs. 14, 15. At the excitation
frequency of 12 kHz, the drill excitation amplitude becomes maximum, but
tool holder amplitude stays relatively low (Fig. 14). In contrast, at
the excitation frequency of 16.6 kHz, drill excitation amplitude becomes
maximum as well as the response of the tool holder, measured at the end
of the concentrator. During vibrational cutting process drill vibrations
are damped at the contact point between the tool and workpiece therefore
the energy transferred from the tool holder may be insufficient.
[FIGURE 13 OMITTED]
[FIGURE 14 OMITTED]
[FIGURE 15 OMITTED]
At the excitation frequency of 16.6 kHz, drill excitation amplitude
becomes maximum and the tool holder excitation reaches peak value as
well. At the second resonant frequency the drilling tool transfers the
highest energy to the drill, thereby leading to the largest positive
influence of vibration drilling.
5. Conclusions
1. Testing revealed that surface roughness during vibrational
drilling decreased up to 25% when compared to conventional drilling.
2. At the first resonant frequency (12 kHz) no appreciable
vibrational drilling influence was observed with respect to conventional
drilling. During tool excitation at the second resonant frequency (16.6
kHz) a significant reduction of cutting force was observed: axial force
decreased in the range of 12-46%, and the torque - 13-20%.
3. At the excitation frequency of 16.6 kHz the tool executes
torsional and longitudinal vibrations, which results in maximal
reduction of both cutting force and torque as well as workpiece surface
roughness. Excitation at this frequency allows to transmit the highest
amount of energy from the tool holder to the drill. This manifests in
the highest observable positive effect of the vibration drilling.
Acknowledgments
This research was funded by a grant (No. MIP113/2010) from the
Research Council of Lithuania. The authors also express their gratitude
for the support of the EGIDE young researchers assistance program.
References
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Received January 04, 2011 Accepted June 30, 2011
M. Ubartas, Kaunas University of Technology, Studentu str. 65,
51367 Kaunas, Lithuania, E- mail:
[email protected]
V. Ostasevicius, Kaunas University of Technology, Studentu g. 65,
51367 Kaunas, Lithuania, E- mail:
[email protected]
S. Samper, Polytech'Annecy-Chambery, 74944 Annecy Le Vieux
Cedex, France, E-mail:
[email protected]
V. Jurenas, Kaunas University of Technology, Kestucio str. 27,
44312 Kaunas, Lithuania, E-mail:
[email protected]
R. Dauksevicius, Kaunas University of Technology, Studentu str. 65,
51367 Kaunas, Lithuania, E-mail:
[email protected]
Table
Main characteristics of the vibrational
drilling tool
Specification Value
Excitation power 200 W
Resonant frequencies 12.0 kHz,
16.6 kHz
Horn material Steel
Twist drill diameter 10 mm
Maximum amplitude 20 [micro]m