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Advances in Materials Science and Engineering
Volume 2013 (2013), Article ID 352173, 7 pages
An Experimental Study on Heat Conduction and Thermal Contact Resistance for the AlN Flake
Department of Mechanical Engineering, Kun Shan University, Tainan 710, Taiwan
Received 24 August 2013; Accepted 17 October 2013
Academic Editor: Teen-Hang Meen
Copyright © 2013 Huann-Ming Chou et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
The electrical technology has been a fast development over the past decades. Moreover, the tendency of microelements and dense division multiplex is significantly for the electrical industries. Therefore, the high thermal conductible and electrical insulating device will be popular and important. It is well known that AlN still maintains stablility in the high temperature. This is quite attractive for the research and development department. Moreover, the thermal conduct coefficient of AlN is several times larger than the others. Therefore, it has been thought to play an important role for the radiator of heat source in the future. Therefore, this paper is focused on the studies of heat conduction and thermal contact resistance between the AlN flake and the copper specimens. The heating temperatures and the contact pressures were selected as the experimental parameters. According to the experimental results, the materials are soft and the real contact areas between the interfaces significantly increase under higher temperatures. As a result, the thermal contact resistance significantly decreases and the heat transfer rate increases with increasing the heating temperature or the contact pressures.
The electrical technology has been a fast development during the first decade of the 21st century. Moreover, the tendency of microelements and dense division multiplex is significantly attractive for the research and development department. To achieve the above goals, the high heat dissipative and electrical insulating device will be popular and important in the future.
It is well known that AlN still maintains stablility under the high temperature conditions. Moreover, the thermal conduct coefficient of AlN material is several times larger than the other nonmetallic solids [1–3]. Hence, it is widely used for the heat dissipation. Besides, AlN film has good electrical insulating properties to avoid the risk of a short circuit of electronic components [4–7]. These advantages are quite attractive for the research and development department of the electrical corporations .
The method of using continuous variations of triboelectrification and friction coefficient to monitor the dynamic tribological properties between the metal films has been applied successfully by the authors [9–12]. The related results also showed that the thermal contact resistance of the metal films is significantly influenced by the real contact areas between the interfaces. Moreover, the major factors for the real contact areas are the normal loads and the surface hardness of the materials. On the other hand, the defects of the material crystal always play an important role for the heat transfer of AlN [1–7]. Therefore, the relationships between the microstructures of AlN film and the efficiency of the heat transfer are the key points. Based on the above statements, this paper is focused on the studies of heat conduction and thermal contact resistance between the AlN flake and the copper specimen by referring the previous studies of thermal contact resistance between the metal films.
2. Experimental Apparatus and Procedures
2.1. Experimental Apparatus
The schematic diagram of thermal contact resistance tester with measuring system is shown in Figure 1. The voltage signals from each measurement point of the thermocouples were transferred to the temperature extractor. There are ten thermocouples in the systems. The temperatures at the measuring point can be obtained by the calibration. Then, the thermal contact resistance and the heat transfer rate can be obtained by the three mathematical formulas as shown in Section 2.3.
Figure 2 shows the main parts of the experimental apparatus. The loading systems contain the following: one-way pneumatic valve manual control, with a model DJA25N75 pneumatic cylinder, and 1HP air compressor.
The main heat transfer gateway is made of copper: heat transfer stick (Φ20 mm × 110 mm, drilling Φ1.4 mm × deep 10 mm) × 2; copper substrate (Φ20 mm × 20 mm, drilling Φ1.4 mm × deep 10 mm) × 1.
The insulation equipment is made of ceramic glass fiber cotton ( W/m°C). The heating equipment includes the three heating rods (CIR-2034/240 V). Several counterweights (1 kgw × 3, 5 kgw × 2, and 10 kgw × 1) are used for maintaining the equilibrium of the contact pressure. Moreover, the water circulating pump and the ice water maker are disposed for the temperature control.
2.2. Test Specimens
AlN thin flakes were used as the main experimental specimens. Material properties are shown in Table 1. The thickness of AlN slices is only 0.7 mm. The size and shape of the specimens are shown in Figure 3(a). AlN slices, and copper specimen, and the heat transfer rod are shown in Figures 3(b) and 3(c).
2.3. Experimental Procedures
There are two types of thermal contact resistance in this study. The upper measuring point of the heat transfer rod is and the lower is . Several parameters influence and , such as temperature, pressure, material, and surface roughness. Therefore, it is necessary to clarify and calculate them step by step.
The formula of the heat transfer is The formula of the thermal contact resistance is Moreover, the related temperatures are obtained by the following:
The heating temperatures were set at 50°C, 65°C, 80°C, and 100°C. The temperature of the ice water circulating system was fixed at 10°C. Before each test, the preparatory time was set at 4 hours. The normal loads were set at 0.5 kgw and 1.5 kgw, and the corresponding contact pressures were 16 kPa and 48 kPa. The average room temperature for the test was °C, and the average relative humidity was %.
3. Results and Discussions
Figure 4 shows the effects of the heating temperature on the thermal contact resistance for Cu/AlN/Cu under 16 kPa. It is seen from this figure that and are independent of the heating temperatures and the experimental time for the temperatures is larger than 50°C. maintains about 1°C/W and maintains about 2.2°C/W for the higher temperatures. Moreover, increases from 0.7°C/W to 0.91°C/W and increases from 1.8°C/W to 2.2°C/W with the experimental time for the heating temperature of 50°C.
The effects of the heating temperature on the heat transfer rate for Cu/AlN/Cu under 16 kPa are shown in Figure 5. It is seen from this figure that the heat transfer rate increases from 10 W to 19 W with increasing the heating temperature from 50°C to 100°C.
Figure 6 shows the effects of the heating temperature on the thermal contact resistance for Cu/AlN/Cu under 48 kPa. It is seen from Figure 6(a) that the increasing trends are similar to the cases of 16 kPa except 100°C. The thermal contact resistance especially decreases with the experimental time under 100°C and 48 kPa. This indicates that the materials are soft under the higher temperatures. As a result, the real contact areas between the interfaces significantly increase. Hence, the thermal contact resistance significantly decreases.
The effects of the heating temperature on the heat transfer rate for Cu/AlN/Cu under 48 kPa are shown in Figure 7. It is seen from this figure that the heat transfer rate increases from 10 W to 17 W with increasing the heating temperature from 50°C to 80°C. Moreover, the heat transfer rate especially increases to 22~25 W under 100°C and 48 kPa.
Comparing to the cases of Cu/Cu, the thermal contact resistance doubles and the heat transfer rate increases 33% with AlN flake under 50°C and 16 kPa. When the heating temperature increases to 100°C, the thermal contact resistance decreases slightly and the heat transfer rate decreases about 40% with AlN flake.
According to the SEM of AlN-flake surface shown in Figure 8, they are rough and uneven. Moreover, the aspects are in the range of 1~10 μm. Hence, many gaps exist between the interfaces. That is, when the copper is soft under the higher temperatures and contact pressures, it will get into the gaps and the real contact areas between the interfaces significantly increase. Therefore, the thermal contact resistance especially decreases under the higher temperatures and contact pressures. The corresponding results can be observed in Figures 4 and 6.
The thermal contact resistance and the heat transfer rate between Cu/AlN/Cu were experimentally investigated in this study. From the experimental results, the following conclusions were drawn.(1)The materials are soft and the real contact areas between the interfaces significantly increase under the higher temperatures. As a result, the thermal contact resistance significantly decreases and the heat transfer rate increases with increasing the heating temperature.(2)The thermal contact resistance doubles and the heat transfer rate increases 33% with AlN flake under 50°C and 16 kPa. When the heating temperature increases to 100°C, the thermal contact resistance decreases slightly and the heat transfer rate decreases about 40%.(3)The thermal contact resistance significantly decreases and the heat transfer rate increases 4% with AlN flake under 100°C and 48 kPa.
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
The authors would like to express their appreciation to the National Science Council in Taiwan for their financial support under Grant nos. NSC 101-2221-E-168-014 and NSC 102-2622-E-150-002-CC2.
- M. I. Nieto, R. Martínez, L. Mazerolles, and C. Baudín, “Improvement in the thermal shock resistance of alumina through the addition of submicron-sized aluminium nitride particles,” Journal of the European Ceramic Society, vol. 24, no. 8, pp. 2293–2301, 2004.
- J. H. Edgar and W. J. Meng, Properties of Group III Nitrides, 1993.
- Y. Kurokawa, K. Utsumi, and H. Takamizawa, “Development and microstructural characterization of high-thermal-conductivity aluminum nitride ceramics,” Journal of the American Ceramic Society, vol. 71, no. 7, pp. 588–594, 1988.
- X. Xu, H. Wu, and Z. Jin, “Studies of the structure and surface roughness of AlN thin films,” Rare Metal Materials and Engineering, vol. 29, no. 6, pp. 394–397, 2000.
- B. Qiao, Z. Liu, and Y. Li, “Effect of technical parameters on deposition rate of AlN films prepared by magnetron reactive sputtering,” Journal of Northwestern Polytechnical University, vol. 22, no. 22, pp. 260–263, 2004.
- J. Zhang, W. Wang, X. H. Zeng, Y. Z. Shi, and H. Q. Fan, “Fabrication and dielectric property of polymer-matrix composites containing AlN particles for electronic substrates,” Journal of Aeronautical Materials, vol. 26, no. 3, pp. 341–342, 2006.
- Y. D. Wang, H. P. Zhou, L. Qiao, H. Chen, and H. B. Jin, “Thermal conductivity of AlN/PE composite substrate,” Journal of Inorganic Materials, vol. 15, no. 6, pp. 1030–1036, 2000.
- Y. C. Lin, Processing parameters on the performance of aluminum nitride [M.S. thesis], Department of Mechanical Engineering, National Taiwan University of Science and Technology, 2005.
- Y. P. Chang, “A novel method of using continuous tribo-electrification variations for monitoring the tribological properties between pure metal films,” Wear, vol. 262, no. 3-4, pp. 411–423, 2007.
- Y. P. Chang, H. M. Chou, R. F. Horng, and H. M. Chu, “Another method of using dynamic tribo-electrification mechanisms for measuring gas flowrate,” Proceedings of the Institution of Mechanical Engineers J, vol. 221, no. 4, pp. 479–487, 2007.
- Y. P. Chang, Y. C. Chiou, and R. T. Lee, “Tribo-electrification mechanisms for dissimilar metal pairs in dry severe wear process. Part I: effect of speed,” Wear, vol. 264, no. 11-12, pp. 1085–1094, 2008.
- Y. P. Chang, Y. C. Chiou, and R. T. Lee, “Tribo-electrification mechanisms for dissimilar metal pairs in dry severe wear process. Part II: effect of load,” Wear, vol. 264, no. 11-12, pp. 1095–1104, 2008.