3.1. Experimental system and conditions
As shown in Fig. 2, the experimental system mainly includes a pulsed power supply, an XY-axis motion platform, a high-speed rotation pneumatic spindle fixed on a Z-axis platform, an electrolyte circulation system, a high-speed camera, and a CNC system. The pulsed power supply can output the minimum pulse width of 1 µs. The tool electrode uses an end-milling tool, and the auxiliary electrode is made of graphite. The XY-axis motion platform has the displacement resolution of 1 µm and the positioning accuracy of ± 2 µm. The Z axis has the positioning accuracy of ± 0.2 µm, which is equipped with a high-speed pneumatic spindle with the rotation speed up to 50,000 r/min. The pneumatic spindle has the special advantage as conducting the pulsed electricity by its internal conductive parts instead of a traditional electric brush, avoiding the brush force interference on dynamic balance of high speed rotation. In this way, the high-speed rotation and electricity conduction can be acted on the tool electrode when the rotation is driven by the air pressure instead of a traditional motor. The tool electrode is a micro end-milling tool made of tungsten steel with a diameter of 500 µm. The electrolyte circulation system can circulate electrolyte solution to keep its consistent depth. The high-speed camera can shoot a video with the frame up to 15,000 fps and the maximum resolution of 1920×1080. The CNC system is composed of an industrial computer and a programmable multi-axis controller. During the hybrid process of ECDM-HSM, the voltage and current waveforms are recorded by an oscilloscope with a current sensor.
Table 1 presents the physical properties of the tool electrode. Table 2 presents the workpiece material properties of quartz glass. During the experimental process, the profile and accuracy of the machined grooves is observed and measured by an optical microscope, a white light interference profiler (WLIP), and a scanning electron microscope (SEM). The experimental parameters are presented in Table 3.
Table 1
Physical properties of tool electrode.
Parameter | Description |
Melting point (℃) | 2850 |
Rockwell hardness (HRA) | 90 |
Resistivity (Ω∙m) | 2×10− 7 |
Diameter (µm) | 500 |
Thermal conductivity (Wm− 1K− 1) | 50.2 |
Table 2
Workpiece material properties of quartz glass.
Parameter | Description |
Elastic modulus (GPa) | 72 |
Shear modulus (GPa) | 31 |
Density (g/cm3) | 2.2 |
Tensile strength (MPa) | 48.5 |
Compressive strength (MPa) | 1060 |
Poisson ratio | 0.17 |
Basic experiments are carried out for studying the key processes of gas film formation, discharging behavior, and machining characteristics. Firstly, a digital camera (Fig. 3) and a high-speed camera are used to observe the formation and morphology of bubbles/gas films under high-speed rotation of tool electrode. Secondly, a CCD (charge coupled device) camera is adopted to observe the discharging phenomenon on the tool surface. The influence of applied voltage, tool rotation speed, and electrolyte concentration on the discharging behavior is analyzed for selecting the optimal parameters. At last, the machining experiments of grooves on quartz glass are carried out to compare ECDM-HSM with HSM with a relative large cutting depth of 200 µm. By obtaining the effect of the tool feed rate, tool rotation, and applied voltage on the size, shape, overcut rate, and surface roughness, the processing mechanism of ECDM-HSM is analyzed. A typical groove as an example is machined to demonstrate the optimal effect.
Table 3
Parameter | Hybrid process of ECDM and HSM | HSM |
Material of end-milling tool | Tungsten steel |
Rotation speed | 5,000 r/min, 8,000 r/min, 10,000 r/min, 20,000 r/min, and 30,000 r/min |
Feed method | Constant feed rate |
Electrolyte | NaNO3 (1wt%, 5wt%, 10wt%, and 20wt%) |
Interelectrode voltage | 100–200 V | - |
Pulse width/pulse interval | 16 µs/8 µs | - |
Tool diameter | 0.5 mm |
Immersion depth | 2 mm |
3.2. Effect of key parameters on bubbles and discharging behavior
Figure 4 shows the morphology of bubbles and gas films at different tool rotation speed. When the rotation speed v was 0 rpm, most of larger bubbles gathered on the tool surface to form a thicker gas film, and a few smaller bubbles merged into the large bubbles away from the tool (Fig. 4a). When v = 3,000 r/min, the bubbles separated from the tool surface and spread out quickly (Fig. 4b). When v = 20,000 r/min, the bubbles on the tool electrode surface were thrown out at high speed along the tangential direction under the centrifugal force of the high-speed rotation (Fig. 4c). With the increase of rotation speed, the bubbles were difficult to concentrate near the tool surface. Figure 5 shows the microscopic and instantaneous process of bubbles under the liquid surface, observing by the high-speed camera. When v = 0 rpm, the bubbles gradually grew up with electrochemical reaction to form a thin gas film. Continuing the electrochemical reaction, a number of smaller bubbles grew and merged into the larger bubbles in the liquid. These larger bubbles caused the uneven thickness of the gas film, which could affect the discharging stability of ECDM. When v = 20,000 r/min, the bubbles gradually formed a "mushroom cloud" shaped air film under the combined effect of the centrifugal force and bubble buoyancy force come from the spiral groove sidewall of the end-milling tool. Although the "mushroom cloud" had a larger range, the bubbles that make up the gas film were smaller and denser compared with that of v = 0 rpm. Moreover, a favorable phenomenon was found that the thickness of the gas film at the end of the tool was thinner and denser, which would facilitate the discharging breakdown there during ECDM process. That is, the advantageous effect of concentrating the discharges to the tool end can be expected.
Figure 6 shows the discharging effect under various conditions of tool rotation speed (0–20,000 rpm), applied voltage (110–160 V), and electrolyte concentration (1wt%, 5wt% and 20wt%). Comparing the horizontal rows in Fig. 6, the discharging phenomenon occurred with the voltage increase until exceeding a critical voltage. Due to the sharp-edge discharging characteristic [11], the discharges firstly occurred at the tip and cutting edge of the tool. As the voltage gradually increased, the discharging area gradually spread upward and covered the lateral cutting edge almost. Comparing the longitudinal columns in Fig. 6, in the case of high-speed rotation, a higher voltage was required to achieve the discharges. We believe that the result is related to the “mushroom cloud” shaped gas film formed by the tool high-speed rotation (Fig. 5). The large centrifugal force caused the bubbles to leave the tool surface quickly, thereby accelerating the H2-gas dissipation so as to be difficult to form a stable insulating film [12]. The higher voltage can speed up the formation rate of electrolytic bubbles for compensating the gas dissipation. When the bubbles formed fast enough to form a gas film, the discharges occurred. Comparing Fig. 6(a) with Fig. 6(b), when the concentration increased from 1wt% to 5wt%, there was no change of the critical voltage. The discharges at the 5wt% concentration looks brighter than that at the concentration of 1wt%, indicating that the larger concentration can bring the denser discharges. Comparing Fig. 6(b) and Fig. 6(c), when the electrolyte concentration was further increased to 20wt%, there was a discharging suppression phenomenon (more difficult to generate discharges), especially for the rotating speed of 20,000 r/min. When the speed was 10,000 r/min and the voltage was 150 V, the discharges only occurred at the electrode tip (as shown in Fig. 6(c)b-5). The experiments found there was not obvious discharges on the tool surface under the condition of the rotation speed ≥ 20,000 r/min (for example Fig. 6(c)a-6).
Figure 7 shows the voltage-current curves and discharging waveforms. The peak voltage and the peak current increase with the increase of applied voltage, and the critical voltage (point I, II, III and IV) increased with the increase of the tool rotation speed. The critical voltage was 120 V at the speed of 0 rpm, while the critical voltage increased up to 135 V, 140 V, and 145 V at the speed of 3,000 r/min, 10,000 r/min, and 20,000 r/min respectively. If the rotation speed was higher, the applied voltage required to be higher in order to achieve the same peak voltage and peak current during ECDM. For example, aiming at the peak current of 1.4 A, the applied voltage needed to reach 145 V at the rotation speed of 20,000 r/min, compared with 120 V at the rotation speed of 0 r/min.
The critical voltages at different electrolyte concentration and different rotation speed are summarized in Fig. 8. The voltages increase with the increase of rotation speed regardless of the electrolyte concentration. In other words, the discharges began more difficult if the rotation speed was higher. However, the excessive peek voltage could make the peak current increase sharply, resulting in excessive overcutting and surface damage caused by the instantaneous huge energy. Therefore, the preferred applied voltage should be slightly higher than the critical voltages to avoid the excessive peak current. According to Fig. 8, the 5wt% concentration of NaNO3 electrolyte is selected for the following machining experiments because its critical voltage is relatively lower at the condition of high rotation speed.
3.3. Machining experiments for comparing HSM with ECDM-HSM
Figure 9 shows the machined results measured by WLIP with the lower feed rate of 0.01 mm/s and 0.05 mm/s at the cutting depth of 200 µm. As known from the HSM results (Fig. 8a1-5 and b1-5), with the increase of rotation speed, the machined surface quality was improved by observing the milling mark and surface roughness Ra. For example, the best result of surface roughness Ra <1 µm (Fig. 9a5) without obvious microcracks was obtained at the speed of 30,000 r/min and the feed rate of 0.01 mm/s. However, the feed rate of 0.05 mm/s resulted in the rougher surfaces and the larger overcutting edges. As for the ECDM-HSM results (Fig. 9A1-5 and B1-5), the width of grooves machined by ECDM-HSM under the combined energy fields was larger than that machined by HSM. The lateral overcutting of 5,000 r/min & 120V and 8,000 r/min & 130 V was 14 µm and 24 µm, respectively. When the rotation speed was higher than 10,000 r/min, the overcutting was sharply increased, and there was a serious surface damage. We believe two possible reasons causing this result. First, the discharging critical voltage was higher corresponding to the higher rotating speed, therefore a larger discharging energy caused the excessive removal of workpiece material (e.g. Figure 9A5). Second, the higher rotating speed led to the unstable gas film, resulting in the unstable energy distribution of the discharges. This is easy to cause the centralized discharges in some positions, which produced the large pits and the unregulated shape of the grooves. In the case of same rotation speed, the lateral overcutting and the machined depth (Fig. 9B1-5) at the feed rate of 0.05 mm/s were smaller than that (Fig. 9A1-5) of 0.01 mm/s, which can be interpreted as the higher feed rate can disperse the discharge energy over a larger area in unit time.
Furthermore, the comparison experiments were carried out by increasing the feed rate. Figure 10 shows the machined results measured by WLIP with the higher feed rate of 0.1 mm/s and 0.5 mm/s at the cutting depth of 200 µm. Compared with the results at lower feed rates of 0.01 mm/s and 0.05 mm/s (Fig. 9), the machined accuracies of 0.1 mm/s and 0.5 mm/s were significantly improved by the hybrid process of ECDM-HSM. Even with the larger discharging energy (160 V and 180 V), the heat damage areas on groove edges were reduced obviously. When the feed rate was 0.1 mm/s, the surface roughness at different rotation speed was basically same as Ra 2.1 µm. When the feed rate was 0.5 mm/s, the surface roughness (Fig. 10B1-5) was almost better than that (Fig. 10A1-5) of 0.1 mm/s. In contrast, the edge break and the tool milling marks in HSM become more serious than that in ECDM-HSM. The HSM process was probably in brittle cutting stage of quartz glass, resulting in the deteriorative surface roughness (for example, Ra 2.6 µm in Fig. 10b-1). According to the comparison, ECDM-HSM can change the brittle cutting into the plastic cutting under the combined action of discharging temperature and chemical reaction, so as to improve the processing effect of the machined accuracies.
The width and the depth of the machined grooves by ECDM-HSM are summarized in Fig. 11. The overcutting under a low feed rate has unfavorable effect on the groove width and depth. With the increase of feed rate, the machined accuracy was significantly improved. As for the cases of rotation speed 10,000–20,000 rpm under feed rate 0.5 mm/s, the errors of groove width and groove depth can be controlled < 10 µm and < 5 µm respectively. Therefore, the optimized strategy of ECDM-HSM was proposed as the idea of a high feed rate with a favorable high-speed tool rotation for equilibrating the combined energy of electrical discharge erosion, electrochemical dissolution, and mechanical cutting. This goal is to avoid the excessive concentration of electrical discharge energy and achieve the state of plastic cutting.
The machining experiments were further carried out by increasing the feed rate. Figure 12 summaries the relationship between feed rate and surface roughness. As for the lower feed rate (≤ 0.05 mm/s), the surface quality of ECDM-HSM was obviously worse than that of HSM due to the high temperature damage from the discharging overconcentration. Under the condition of higher feed rate (≥ 0.1 mm/s), the surface quality of ECDM-HSM was improved significantly and better than that of HSM owing to the effect of the combined energy fields. Using the process of ECDM-HSM at the feed rate of 0.5 mm/s, the value of surface roughness Ra can reach the best one as 1.7 µm (tool rotation 10,000 r/min). Moreover, the improved effect of ECDM-HSM was more obvious in the case of the higher feed rate. Taking the feed rate of 1.0 mm/s (tool rotation 10,000 r/min) as an example, the surface roughness Ra can be improved from 6.3 µm of HSM to 3.0 µm of ECDM-HSM, although the surfaces become worse in both processes of ECDM-HSM and HSM compared with that of 0.5 mm/s. In other words, given the similar surface roughness and accuracy, the hybrid process of ECDM-HSM can apply higher feed rate for improving machining efficiency. Considering the similar surface quality by comparing the case of 0.01 mm/s and 10,000 r/min (Fig. 9a-3) with the case of 0.5 mm/s and 10,000 r/min (Fig. 10B-3), ECDM-HSM can improve the processing efficiency by 50 times more than that of HSM. In contrast to the ECDM machining efficiency of existing experimental result as Ra ~2µm [8], that of ECDM-HSM can improve by 10 times. The hybrid process of ECDM-HSM can better balance the processing accuracy and efficiency.