ABSTRACT

Striation-free laser cutting, especially for thick section steel, is hard to obtain due to several factors. The inside shape of the gas nozzle is considered to be one of the most vital factors in striation-free fiber laser cutting. 0.8 mm normal nozzle and a supersonic nozzle are used to cut 0.8 mm AISI316L stainless steel (0₂₂Cr₁₇Ni₁₂Mo₂) separately. The orthogonal experiment takes nozzle standoff distance, cutting speed, Laser power and gas pressure as its impacting factors. The same orthogonal table is adopted in different condition, using normal nozzle and using supersonic nozzle. In the mean time, Ar gas is used as assisted cutting gas in the experiment. The data from this experiment show that supersonic nozzle seems to be a strong helper for fiber laser cutting. Feed rate’s effect seems stable and inconspicuous under the condition of using supersonic nozzle.

Keywords:

Fiber Laser Cutting, Stainless Steel, Striation, Supersonic Nozzle

1. Introduction

Striation-free laser cutting, especially for thick section steel, is hard to obtain due to several factors. There are quite a few scholars who were engaged in this issue recently. People believed that the inside shape of the gas nozzle is considered to be one of the most vital factors during striation-free fiber laser cutting [1] - [25] .

Nozzle’s function in laser cutting is considered as assisting cutting process. Normal nozzle seems to be easy causing unstable gas flow which is one of the probabilities to generate striation. So many scholars pay more attention to design of supersonic gas nozzle. Figure 1 shows the short cutting structure of supersonic nozzle. This structure was studied by Guo Shaogang et al. (2007) [26] , which can obtain the uniform flow and the optimum dynamic characteristic and is easier to be made than before.

However, people still doubt about which kind impact of this kind of supersonic nozzle. So what we interested here is try to test the purpose of the inside shape of the gas nozzle which is considered to be one of the most vital factors in striation-free fiber laser cutting. 0.8 mm normal nozzle and a supersonic nozzle, which was modified of 0.8 mm normal nozzle, are used in this experiment. The orthogonal experiment takes nozzle standoff distance, cutting speed, Laser power and gas pressure as its impacting factors. The same orthogonal table is adopted in each condition.

2. Experimental Procedures

2.1. The Laser System and Cutting Material

The work pieces used in the experiments were as-received 0.8 mm thick AISI316L stainless sheets (0₂₂Cr₁₇Ni₁₂Mo₂). Laser cutting experiments were conducted using a 1 kW continuous wave (cw) IPG YLR-1000-SM ytterbium single-mode fiber laser with 1.07 μm wavelength, a TEM00 beam intensity distribution, and a 14 μm delivery fiber core diameter. The beam has an M2 of 1.1. After the delivery optical fiber, the laser beam was collimated to a 3 mm diameter and focused using a lens of 7.5 inch focal length. The laser beam spot size at focus was measured to be 62 μm. During laser cutting experiments the laser power was varied between 800 and 1000 W and the cutting speed between 10 and 30 mm/s. Focal position was varied between 5 mm below the work piece surface, and 13 mm above the surface.

A Practice laser cutting head with a coaxial conical nozzle and a 0.8 mm exit hole diameter was used. The nozzle standoff from the work piece was varied between 1 and 2 mm. The work piece was placed on a CNC x-y table below the stationary laser beam as shown in Figure 2. Ar gas was used with the regulator gas pressure set between 1.0 and 2.0 bar. The laser cut samples were analyzed by using an optical microscopy.

2.2. Inside Shape Supersonic Nozzle

There is a coaxial conical nozzle and a 0.8 mm exit hole diameter inside normal cutting head. Normal nozzle does not have a throat, while supersonic nozzle should have a throat near the end of gas outlet. So the supersonic nozzle was modified from normal cutting nozzle. There is a chamfer at the end of its exit hole which could be shown in Figure 3. The diameter dc is 1.76 mm, and diameter do is 2.26 mm and LO is 2.0 mm.

2.3. The Optimization Algorithm

There are four controlling factors in this optimization algorithm experiment. Table 1 shows their levels in details used in experimentation.

Table 2 shows the standard L4³ test schedule which was used in laser cutting with normal nozzle as well as supersonic nozzle.

3. Results

3.1. Synthesis Analysis

In this optimization algorithm, roughness, which could be measured by using a LSM 700 3D Laser Scanning Microscope on the cutting section of each sample, is considered as the index of evaluation of the analysis by synthesis. According to specific circumstance, the calculation formula shows below.

(1)

In Formula (1), i stands for test piece number; T_i stands for roughness; T_max stands for the maximum roughness; T_min stands for the minimize roughness; K_i stands for synthesize analysis score of each sample.

3.2. Range Analysis

Range analysis can be used to calculate the range R, using mathematical statistics to work out, in each collar of orthogonal table; and the primary and secondary relationship of every factor could be based on its value. According to the value of the range, people can look for reasonable combining parameters of fiber cutting machine. The calculation formula shows below.

(2)

In Formula (2), subscript j stands for level of the optimization algorithm; k stands for impacting factor of the optimization algorithm. ΔR equals to the Maximum among I, II, III in K collar minus the Minimum among I, II, III in K collar inside Table 3.

3.3. Analyzing Relationship between Factors and Indexes under the Condition of Using 0.8 mm Nozzle

(1) Analyzing datum inside Table 2, the 8th test sample seems the best one, to which its level combing is A₃B₂C₁D₃; the 6th test sample seems the worst one, to which its level combing is A₂B₃C₁D₂.

(2) The primary and secondary relationship of 4 factors in Table 3 and Figure 4 shows their rank order: D → B → A → C. Factor D could be found that its impact dominated among the four factors. A, B and C factors’ effect seems that there was so little difference between them.

3.4. Analyzing Relationship between Factors and Indexes under the Condition of Using 0.8 mm Supersonic Nozzle

(1) Analyzing datum inside Table 4, the 2th test sample seems the best one, to which its level combing is A₁B₂C₂D₂; the 7th test sample seems the worst one, to which its level combing is A₃B₁C₃D₂. But, its score can compare with average score under the condition of using 0.8 mm normal nozzle.

(2) The primary and secondary relationship of 4 factors in Table 5 and Figure 5 shows their rank order: A → B → C → D. Factor A could be found that its impact dominated among the four factors. B, C factors’ effect seems that there was so little difference between them. Factor D’s effect seems stable and inconspicuous under the condition of using supersonic nozzle.

4. Discussion

There are some differences between normal nozzle laser cutting and supersonic nozzle laser cutting. The primary and secondary relationship between 4 factors of two different conditions is absolutely different. Supersonic nozzle may get a stabilized gas flow, and the stable gas flow can even obtain at a relatively higher feed rate. This is the reason why the total score of test samples inside Table 4 is higher than that inside Table 2.

The range of D factor (feed rate) becomes small when supersonic nozzle is used. This is another clue that shows supersonic nozzle could obtain a relative stable gas flow.

However, there is a same result between normal nozzle laser cutting and supersonic nozzle laser cutting. The best properly combined parameters is A₁B₂C₂D₁. The tendency of factor A, B and C in different conditions seems similar.

There are more than 4 factors which can affect the cutting quality, and may result in striation on the section of work pieces. The value of different level of each factor inside the optimization algorithm is setted according to real condition of fiber laser cutting such as thickness of stainless steel and the type of fiber cutting machine. The supersonic nozzle using here does not have an arc shape at convergence section showing in Figure 1. These limitations will make the result, which we get before, uncertain.

5. Conclusions

Supersonic nozzle seems to have two functions. One is that it could weak the impact of feed rate in fiber laser cutting of stainless steel; the other is that it could improve cutting quality of stainless steel fiber laser cutting. These functions could be useful for application of fiber laser cutting.

Whichever kind of nozzle is used in fiber laser cutting, tendency of factor A, B and C to cutting quality is similar. According to this result, it is accessible to obtain reasonable combine parameters by optimization algorithm. There is a same result between normal nozzle laser cutting and supersonic nozzle laser cutting. The best properly combined parameters seems to be A₁B₂C₂D₁ here.

Supersonic nozzle may be better than normal nozzle if we plan to eliminate the striation on the section of work pieces in fiber laser cutting.

Cite this paper

Zhou, Y.J., Kong, J.L. and Zhang, J. (2017) Study on the Role of Supersonic Nozzle in Fiber Laser Cutting of Stainless Steel. Materials Sciences and Ap- plications, 8, 85-93. http://dx.doi.org/10.4236/msa.2017.81006

References