Handbook of Advanced Ceramics Machining Episode 11 pot

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Handbook of Advanced Ceramics Machining Episode 11 pot

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13.4 Experimental Results The main results obtained for the four types of slurries are as follows: 13.4.1 Material Removal For 0.25 mm monocrystalline diamond, we removed 7.395 mm per 12 min of machining or 0.6163 mm per min. This rate is with a different charging method and is showing lesser efficiency than the one described earlier. For 0.25 mm polycrystalline diamond, we removed 15.636 mm per 12 min of machining or 1.303 mm per min. For 0.125 monocrystalline diamond, we removed 3.236 mm per 12 min of machining or 0.2697 mm per min. For 0.125 polycrystalline diamond, we removed 3.575 mm per 12 min of machining or 0.2979 mm per min. It can be seen that on the 0.25 mm slurry, the material removal rate for polycrystalline is twice that for monocrystalline, optimizing production volume and time savings. In the 0.125 mm, the results are quite different; the removal rate is very small (around 9%) compared with the 0.25 mm. In this case, the decision-making process should include other parameters like economy, 60Њ Part FIGURE 13.1 Part location on the experiments. Ioan D. Marinescu/Handbook of Advanced Ceramics Machining 3837_C013 Final Proof page 286 18.10.2006 6:37pm 286 Handbook of Advanced Ceramics Machining availability, and so on. Figure 13.2 shows the graphs for material removed during the experiments. 13.4.2 Roughness and Profile The preliminary results on the AFM show roughness on some parts of about 2 nm on the lower end of the range. The roughness and profile measure- ments are in progress because of a heavy volume of work on the AFM and the priorities assigned to it by the department of chemical engineering (owner of the equipment). This fact does not allow more results to be disclosed now that this report is getting printed. Figure 13.3, Figure 13.4, Figure 13.5, and Figure 13.6 are surface roughness images obtained on the AFM for different parts. Figure 13.7, Figure 13.8, and Figure 13.9 are topog- raphy images of these parts. 13.5 Remaining Work The remaining work includes: . Analysis of the roughness and profile of the parts for the different types of slurries. . Analysis of the effect on the plate surface roughness, it has proven to be of critical importance in these experiments. . Analysis of the part holder material (soft or hard) that also showed itself as an important parameter. 0 10 20 30 11013 Micrometers Average material removed per batch (0.25 µm slurry) Batch number Monocrystalline diamond Polycrystalline diamond 74 FIGURE 13.2 Average material removed (in mm) per batch of six parts. Ioan D. Marinescu/Handbook of Advanced Ceramics Machining 3837_C013 Final Proof page 287 18.10.2006 6:37pm Super Polishing of Magnetic Heads 287 Roughness analysis Peak nonlaped.000 Surface Peak off Summit off Zero cross. Off box cursor Area Summit Zero Crossing Stopband Execute Cursor 100 75 Image statistics Img. Img. Img. Img. Img. Z range mean raw mean Rms (R q ) R a 1.435 nm 0.00002 nm 32.943 nm 94.004 nm 67.034 nm 768.63 nm −37.394 nm −4.452 nm 140.11 nm 107.65 nm 20.176 µm 9.969 µm Z range Mean Raw mean Rms (R q ) Mean roughness (R a ) Box x dimension Box y dimension Box statistics 50 25 0 1007550250 FIGURE 13.3 Image of a nonlapped magnetic head showing the roughness of the full scanned area and the roughness of the small rectangle. Roughness analysis Peak Surface Area Summit Zero Crossing Stopband Execute Cursor 80.0 60.0 40.0 20.0 80.060.040.020.00 s1-25-1.000 0 µm Peak off Summit off Zero cross. Off box cursor Image statistics Box statistics Img. Img. Img. Img. Img. Z range mean raw mean Rms (R q ) R a 919.29 nm 114.64 nmZ range Mean Raw mean Rms (R q ) Mean roughness (R a ) Box x dimension Box y dimension −0.00003 nm −108.76 nm 4.665 nm 17.691 nm −0.555 nm −159.28 nm 3.789 nm 1.538 nm 15.936 µm 6.142 µm FIGURE 13.4 Image of a lapped magnetic head with 0.25 mm slurry, showing the roughness of the full scanned area and the roughness of the small rectangle. Ioan D. Marinescu/Handbook of Advanced Ceramics Machining 3837_C013 Final Proof page 288 18.10.2006 6:37pm 288 Handbook of Advanced Ceramics Machining Roughness analysis Peak Surface Area Summit Zero Crossing Stopband Execute Cursor 100 75 50 25 0 µm 0 25 50 75 100 Image statistics Box statistics Img. Img. Img. Img. Img. Z range mean raw mean Rms (R q ) R a 1.013 µm 998.75 nmZ range Mean Raw mean Rms (R q ) Mean roughness (R a ) Box x dimension Box y dimension Peak off Summit off Zero cross. Off box cursor nonapd2.000 −0.00001 nm −12.810 nm 79.340 nm 54.044 nm –9.159 nm –55.780 nm 99.214 nm 64.097 nm 20.983 µm 13.312 µm FIGURE 13.5 Image of a nonlapped magnetic head showing the roughness of the full scanned area and the roughness of the small rectangle. Roughness analysis Peak Surface Area Summit Zero Crossing Stopband Execute Cursor 100 75 50 25 0 m 0 25 50 75 100 Peak off Summit off Zero cross. Off box cursor 125mos48.000 Image statistics Box statistics Img. Img. Img. Img. Img. Z range mean raw mean Rms (R q ) R a 758.98 nm 87.504 nmZ range Mean Raw mean Rms (R q ) Mean roughness (R a ) Box x dimension Box y dimension 0.000003 nm 26.489 nm 13.637 nm 4.966 nm –0.086 nm 26.403 nm 3.795 nm 1.806 nm 20.900 µm 8.956 µm FIGURE 13.6 Image of a lapped magnetic head with 0.125 mm slurry, showing the roughness of the full scanned area and the roughness of the small rectangle. Ioan D. Marinescu/Handbook of Advanced Ceramics Machining 3837_C013 Final Proof page 289 18.10.2006 6:37pm Super Polishing of Magnetic Heads 289 Digital instruments Scan size Scan rate Number of samples View angle Light angle 0 deg X 20.000 µm/div Z 2.000 µm/div 20 40 60 80 100 120 µm 121.3 µm 1.001 Hz 512 Nanoscope FIGURE 13.7 Image of a nonlapped magnetic head showing the topography of the surface. X 20.000 µm/div Z 1.000 µm/div Digital Instructions Scan size Scan rate Number of samples Nanoscope 121.3 µm 1.001 Hz 512 View angle Light angle 0 deg µm 80 60 40 20 FIGURE 13.8 Image of a lapped magnetic head using 0.25 mm slurry, showing the topography of the surface. Ioan D. Marinescu/Handbook of Advanced Ceramics Machining 3837_C013 Final Proof page 290 18.10.2006 6:37pm 290 Handbook of Advanced Ceramics Machining . Other parameter that might be analyzed is the speed (parts and plate) and its effect on the surface roughness. . The material of the plate is also in the scope of this study. . Use of acoustic emission techniques for the polishing process analysis. Digital instruments Scan size Scan rate Number of samples µm 120 100 80 X Z 20.000 µm/div 1.000 µm/div 60 40 20 Nanoscope 123.7 µm 1.001 Hz 512 View angle Light angle 0 deg FIGURE 13.9 Image of a lapped magnetic head using 0.125 mm slurry, showing the topography of the surface. Ioan D. Marinescu/Handbook of Advanced Ceramics Machining 3837_C013 Final Proof page 291 18.10.2006 6:37pm Super Polishing of Magnetic Heads 291 Ioan D. Marinescu/Handbook of Advanced Ceramics Machining 3837_C013 Final Proof page 292 18.10.2006 6:37pm 14 Laser-Assisted Grinding of Ceramics I.D. Marinescu, T.D. Howes and J. Webster CONTENTS 14.1 Objectives 293 14.2 Problem Statement 294 14.2.1 Introduction 294 14.2.2 Experimental Setup 294 14.2.3 Results and Discussions 295 14.3 Stock Removal Mechanism 297 14.4 Conclusions 299 14.5 Future Directions 299 Bibliography 299 14.1 Objectives The objectives of this chapter are to determine the parameters of a new technology for high productivity, low cost of hot-pressed silicon nitride (HPSN) ceramic materials and to determine if an available grinding wheel system can be used for these applications. Ceramic materials are commonly brittle materials with varying degrees of brittleness. The aim of this research is to increase the ductility of HPSN ceramic materials by the aid of laser preheating process and in process. With this method, it will be possible to increase the depth of cut (productivity of the process) more than 20 times and at the same time, keep the process in the ductile mode (free of surface and subsurface damages). This research is unique in that the grinding system will be considered as a thermal-tribo system and the laser energy and friction energy together will provide indications for the necessary energy for increasing the ductility of HPSN ceramic materials. Ioan D. Marinescu/Handbook of Advanced Ceramics Machining 3837_C014 Final Proof page 293 6.10.2006 2:24am 293 14.2 Problem Statement 14.2.1 Introduction Ceramic materials are considered brittle materials and are examples of difficult-to-grind (machine) materials. This is because of the mechanical properties of these materials, most notably hardness, brittleness, and abra- siveness. Previous research showed that the only way to obtain a good quality ground surface is through ductile grinding of ceramics with dia- mond wheels. But even in this case, the depth of the cut must be less than 1 mm, which makes the process very expensive. Many researchers have tried different solutions and a very successful method was that of high-speed grinding of ceramics, but even in this case the process is very expensive. Ceramic materials are not extensively used in industry because the cost of the machining is very high and represents between 50% and 80% of the cost of the part. We are looking for a solution to reduce the cost through increased productivity. From the experiments done with high-speed grinding, one can observe the effect of the temperature on the quality of the surface and note that an increase in temperature helps in obtaining a better surface and a better pullout. 14.2.2 Experimental Setup Based on this observation, an experiment was done at the Center for Grinding Research and Development at the University of Connecticut. A laser was mounted on a surface grinder to preheat the ceramic surface just before it contacts the grinding wheel (see Figure 14.1). A dynamometer and a thermo- couple were used together with a data acquisition system. The experiment was done for four types of ceramics (Table 14.1): Al 2 O 3 , Ferrite, ZrO 2 , and Si 3 N 3 . The aim of the experiment was to show that it is possible to increase the ductility of ceramics through a preheating process and to increase the depth of cut while the material is in the ductile state. The experiment was done in two steps: (1) grinding of ceramic materials and (2) grinding of ceramic materials preheated with laser under the same experimental condi- tions. During the experiment, the forces and the temperature were measured in process. The experiment parameters were as follows: . Wheel speed: Vs ¼ 25 m=s. . Depth of cut: a ¼ 50 mm. . Work speed: vw ¼ 2mm=s. . Wheel type: 1A1, D400, C75, Resin Bond & Friable Diamond, Kt8821YA. Ioan D. Marinescu/Handbook of Advanced Ceramics Machining 3837_C014 Final Proof page 294 6.10.2006 2:24am 294 Handbook of Advanced Ceramics Machining 14.2.3 Results and Discussions The experimental results are presented in Table 14.1. The normal force (F n ) and tangential force (F z ) were generally higher under the laser preheated condition (Figure 14.2 and Figure 14.3). The behavior of silicon nitride is remarkably unusual. From Figure 14.4, one can see that there are two behaviors for the friction coefficient: in one, the friction coefficient decreases when preheating the ceramics (Ferrite, Zr 2 O 3 ), in the other two materials, the coefficient rises slightly in response to laser preheating. But the most interesting results are shown in Figure 14.5, in which we can see that the roughness of the surface is better for all four types of ceramics when the grinding is done with preheated ceramics. When we look at SEM photos (Figure 14.6 and Figure 14.7) of surfaces ground with and without heat, we see a tendency toward a ductile surface in the case of grinding with preheating. The structure shows some evidence of melting zones, probably at the asperities of the ceramic materials. Converter Thermocouple Diode laser Data aquisition system Dynamometer Charge amplifier A to D Converter Conditioning board FIGURE 14.1 Experimental setup for tests. TABLE 14.1 Experimental Results Workpiece Material Al 2 O 3 w=Heat Ferrite w=Heat ZrO 2 w=Heat Si 3 N 4 w=Heat F n [N] 15 9 2.5 2.0 15 25 10 15 F t [N] 2.5 2.0 0.5 0.25 7 5 5 8 R a 8.2 12.5 12.3 13.6 5.4 6 3.8 4.5 Force Coefficient 0.167 0.222 0.2 0.125 0.467 0.2 0.5 0.53 Ioan D. Marinescu/Handbook of Advanced Ceramics Machining 3837_C014 Final Proof page 295 6.10.2006 2:24am Laser-Assisted Grinding of Ceramics 295 [...]... Conference on Machining of Advanced Material, NIST Special Publications 847, 1993 Ioan D Marinescu /Handbook of Advanced Ceramics Machining 3837_C014 Final Proof page 300 6.10.2006 2:24am 300 Handbook of Advanced Ceramics Machining Marinescu, I.D., Laser assisted grinding of ceramics, CIRP Winter Meeting, January 22–24, 1995, Paris, France Marinescu, I.D., Laser heating in grinding of ceramics, STC-Abrasive...Ioan D Marinescu /Handbook of Advanced Ceramics Machining 3837_C014 Final Proof page 296 6.10.2006 2:24am Handbook of Advanced Ceramics Machining 296 25 20 15 10 5 0 Workpiece heated by laser Unheated workpiece FIGURE 14.2 Normal grinding force FIGURE 14.3 Macro-fracture FIGURE 14.4 Micro-fracture Ioan D Marinescu /Handbook of Advanced Ceramics Machining 3837_C014 Final Proof page 297 6.10.2006... influence of the temperature upon the stock removal mechanism in the case of brittle material, but no one had performed specific research in this area Even the measurement FIGURE 14.6 SEM Image of a ground surface without heat Ioan D Marinescu /Handbook of Advanced Ceramics Machining 3837_C014 Final Proof page 298 6.10.2006 2:24am 298 Handbook of Advanced Ceramics Machining FIGURE 14.7 SEM Image of a ground... the latter 4 The oxidation film on the surface of the cast-iron bond of the diamond wheel has a great influence on wear characteristics and friction coefficient Ioan D Marinescu /Handbook of Advanced Ceramics Machining 3837_C015 Final Proof 312 page 312 2.10.2006 6:18pm Handbook of Advanced Ceramics Machining References Hokkirigawa, K Wear mode map of ceramics, Wear, 1991, Vol 151, pp 219–228 Kato,... is independent of the normal load 15.4 Consideration for ELID-Grinding from the Viewpoint of Tribology Figure 15.9 shows an example of a grinding based on the relationships from Figure 15.5 and Figure 15.8 The following relation can be drawn: G2 > G1 , Ioan D Marinescu /Handbook of Advanced Ceramics Machining 3837_C015 Final Proof page 308 2.10.2006 6:18pm Handbook of Advanced Ceramics Machining 308... The wear process of the wheel was recorded on a video tape recorder The sapphire pin (radius of pin tip: 1 mm, Hv: 2500) was used as a Monitor Normal load 3 1 4 VTR 2 CCD microscope 5 3 FIGURE 15.2 Schematic diagram of the CCD microscope tribosystem Ioan D Marinescu /Handbook of Advanced Ceramics Machining 3837_C015 Final Proof 304 page 304 2.10.2006 6:18pm Handbook of Advanced Ceramics Machining specimen... mm3=mm During the initial friction stage, the friction coefficient in the presence of an oxide film has a higher value than that without an oxide film This is because of the fact 301 Ioan D Marinescu /Handbook of Advanced Ceramics Machining 3837_C015 Final Proof page 302 2.10.2006 6:18pm Handbook of Advanced Ceramics Machining 302 that the wear is higher at initial friction stage than that without an... Marinescu /Handbook of Advanced Ceramics Machining 3837_C015 Final Proof page 310 2.10.2006 6:18pm Handbook of Advanced Ceramics Machining 310 Wear rate w, mm3/mm 1.00E-03 SD400 1.00E-04 1.00E-05 Flake formation SD400 with oxide film 1.00E-06 Plowing or powder formation 1.00E-07 1.00E-08 1 10 100 Contact pressure P, MPa 1000 FIGURE 15 .11 Relationship between contact pressure and wear rate of grinding... model in lapping of ceramics, Proceedings of ASPE, Spring Meeting, June 2–4, Annapolis, MD Marinescu, I.D., Laser assisted grinding of ceramics, Journal of Abrasives, AES, August 1995 Marinescu, I.D., Hot grinding of ceramics, Machining and Grinding of Brittle Materials, Ceramic Industry Conference, 11 13 October 1995 Ueda, T., Thermal behavior of cutting grain in grinding, Annals of the CIRP, Vol... design of auxiliary processes, especially the conditioning of diamond grinding wheels and the selection of suitable cooling lubrication conditions Ioan D Marinescu /Handbook of Advanced Ceramics Machining 3837_C016 Final Proof Developments in Machining of Ceramic Materials page 315 2.10.2006 6:19pm 315 Numerous research studies were conducted during the past few years on ¨ finish machining of ceramic . 11 13, 1991. Ioan D. Marinescu /Handbook of Advanced Ceramics Machining 3837_C014 Final Proof page 300 6.10.2006 2:24am 300 Handbook of Advanced Ceramics Machining 15 Tribological Properties of. mechanisms. Ioan D. Marinescu /Handbook of Advanced Ceramics Machining 3837_C015 Final Proof page 302 2.10.2006 6:18pm 302 Handbook of Advanced Ceramics Machining thickness of the sterilized oxidation. the experiments. Ioan D. Marinescu /Handbook of Advanced Ceramics Machining 3837_C013 Final Proof page 286 18.10.2006 6:37pm 286 Handbook of Advanced Ceramics Machining availability, and so on.

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