Roughness as parameter of cut quality during C[O.sub.2] laser cutting of high alloy steel for the special purpose.
Cekic, Ahmet ; Kulenovic, Malik ; Begic, Derzija 等
1. INTRODUCTION
In the world today, there is rapidly introducing of new
technologies into manufacturing systems from more reasons such as:
saving materials, precision of operation, short processing time, high
accuracy of products and high flexibility. Nowadays laser technologies
are increasingly used in manufacturing and automotive industries. In
most of the use of laser technologies is the laser beam cutting. The
laser beam cutting can be successfully used for the cutting different
materials such as: metals, polymers, ceramics, composites, high alloy
steels and others (Avanish & Vinod, 2008). The use of high alloy
steels in car bodywork has spread in recent years. The AISI institute is
forecasting a dramatic increase in the use of high alloy steels in the
car industry (Lamikiz et al., 2005). In the literature, there are no
more experimental studies of the laser cutting of high alloy steels. The
exothermal reactions of iron and other alloy elements are complex and
high alloy steels have a high content of alloy elements, which can lead
to differences with regard to the cutting of common steels.
Among various types of lasers used for machining in industries,
C[O.sub.2] (wavelength 10.6 um) and Nd: YAG (wavelength 1.06 [micro]m)
lasers are most established in the automotive industries. In order to
use advantages of this technology, especially by aspect of saving
materials is necessary to evaluate the optimum process parameters for
each kind materials, thickness and others process conditions to the
achieving desired cut quality with maximum productivity. The setting of
process parameters mainly depends of the material characteristics
(density, specific heat, absorptivity, thermal conductivity, chemical
composite, surface quality and etc) and thickness of materials. The most
important process parameters are, such as: laser power input, mode of
operation (pulsed mode and continuous wave), pulse frequency, pulse
duration, kind and pressure of assistant gas, focus position, diameter
and kind of nozzle. These parameters are usually determined so those
insure the desired cut quality, and the productivity is less relevant.
The setting of process parameters which would satisfy both the desired
cut quality and high productivity is specific problem (Rajaram et al.,
2003). The quality of the C[O.sub.2] laser cutting was evaluated by a
standard process: measuring of surface roughness, kerf width and kerf
deviation along the length of cut, kerf taper, size of heat affected
zone, micro-hardness and metallographic and etc. Previous work in the
literature elucidated the effects of oxidation dynamics and laser beam
velocity on the quality of the laser cut (Avanish & Vinod, 2008). It
suggested that there is an optimum range of cutting speeds for a given
material, thickness and laser power. Surface roughness is an effective
parameter representing the quality of machined surface. Some researchers
(Nagels et al., 2007) shown that surface roughness value reduces on
increasing cutting speed and frequency, and decreasing the laser power
and gas pressure. Also nitrogen gives better surface finish than oxygen.
In spite of an increase in available laser power during the last decade,
the laser cutting process faces difficulties in cutting thicker parts.
The main problems are losing the process stability and the deterioration
of the cut quality.
2. EXPERIMENTAL PROCEDURE
The preliminary experiments were carried out with a laser system
consisting of a 2800 W continuous C[O.sub.2] laser (Bystronic), a three
axes CNC controlled table with work volume 2.0 m x 1.5 m x 0.5 m.
Experiments were carried out on two different materials with three
thickness of 5, 10, and 15 mm. The chemical compositions of the examined
materials are given in Table 1.
Geometry of the sample shapes are given in Fig. 1. Sample I (EN
10083-3) was previous prepared for laser cutting by using the saw and
milling machine. It was hot rolled square rod with dimensions of
140x140mm. Sample II (GX40CrNiSi22-10) is given from tube, produced by
centrifugal casting.
The beam profile is nearly Gaussian ([TEM.sub.00]) with beam
quality k [approximately equal to] 0.75. Others process parameters were
kept constant throughout the experimentation: the laser power of 2520 W,
the focal length of lens 127 mm, the assistant nitrogen gas pressure of
14 bar, nozzle diameter of 2.0 mm, focus position under bottom side of
sample. Namely, previous experiments are shown that was not possibility
to realize the cutting of tested materials when the oxygen used as
assistant gas. In the previous experiments, the optimal value of
assistant gas pressure and the focus position are obtained. In the
experiments where the laser beam has been focused on the surface of the
sheet and even above the sheet, the results show poor quality in cutting
areas.
[FIGURE 1 OMITTED]
3. ROUGHNESS MEASUREMENT
Surface roughness as parameter of cut quality is analyzed.
Roughness parameter [R.sub.a]--mean deviation is measured. The surface
roughness is measured by using the device Perthometer Concept. DIN 2310
standard prescribed the measuring of surface roughness on the exactly
determined depth. It depends of the material thickness. Because of the
specific process and the obtaining of valid results, the measurements
are performed at the five parallel lines which are uniform sorted along
the depth of cut, Fig.2. Namely, the high of unevenness increase from
the top to the bottom of cut along the length of cut. The exchange of
conditions of the intersection laser beam and material is reason for
that, as and the exchange of the local rate between the thermal
conductivity and the coefficient of absorption (it depends of the
temeparture exchange). Fig. 2 shows the increasing of surface roughness
along the depth of cut in the depending of the process parameters as
well as the kind and the thickness of material. During executing of
experiments, the maximum deviation of 6.6 [micro]m is obtained.
[FIGURE 2 OMITTED]
In the aim of the obtaining of the valid results, the visual
selections of samples are made. The samples with large dross were not
taken in consediration.
4. RESULTS AND DISCUSSION
The experimental values of parameter roughness Ra for different
cutting speeds during laser processing of GX40CrNiSi22--10 steel is
given in Fig. 3 and in Fig.4 for EN 10083 -3 steel.
[FIGURE 3 OMITTED]
[FIGURE 4 OMITTED]
It is observed that, the surface roughness increases by increasing
the material thickness at keeping constant others process parameters
during C[O.sub.2] laser cutting of both examined high alloy steels.
5. CONCLUSION
In this paper are carried out the experimental investigations the
effect of the cutting speed and the thickness of material as well as the
kind and the pressure of the assistant gas on the surface roughness
during the C[O.sub.2] laser cutting two different materials.
Following conclusions can be drawn on the basis of results
obtained:
* Once the correct value has been established, small variations in
pressure do not determine the quality of the cut. Thus, assisting gas
pressure can be maintained for different values of power, cutting speed
and focal position as well as kind and thickness of tested materials.
* Maximum of the possibility cutting speed is depends of the kind
and thickness of material for the given laser system.
Above this maximum there is no possibility to obtain the accepted
level of cut quality.
* Better quality of cut and the large range of cutting speed is
possibility during laser cutting of thinner materials.
In the future work, the influential process parameters during laser
cutting of high alloy steels for the special purpose will be considered.
These process parameters will be optimized with consideration of
multi-performances characteristics of the cut.
6. REFERENCES
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laser cutting of a carbon/carbon multi-lamelled plain-weave structure.
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Avanish, K. D. & Vinod, Y. (2008). Laser beam machining-A
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Lamikiz, A.; Lopez de Lacalle, L. N.; Sanchez, J. A.; Pozo, D.;
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Tab. 1. Chemical compositions of examined materials
Chemical composition of GX40CrNiSi22-10 steel
C Cr Ni Si Mn S P
Min 0,40 18,0 12,0 1,80 ... 0,20 ...
Max 0,70 21,0 14,0 2,20 1,50 0,40 0,06
Chemical composition of EN 10083--3 steel
C Cr Ni Si Mn S P
Min 0,42 1,10 0,05 0,17 0,50 ... ...
Max 0,49 1,40 0,25 0,24 0,80 0,05 0,05