Study on Nano Polyacrylonitrile Fiber by Cotton Candy Method Ryo Takematsu, Masayuki Okoshi, Hiroyuki Inoya and Hiroyuki Hamada, Department of Advanced Fibro-Science, Kyoto Institute of Technology, Gosyokaidocho, Matsugasaki, Sakyo-ku, Kyoto, 606-8585, Japan Akihiro Tada, OHGI TECHNOLOGICAL CREATION CO., LTD. 4-13, 3-chome, Nakano, Otsu City, Shiga Prefecture 520-2114, Japan Yoshifumi Aoi, Department of Materials Chemistry, Faculty of Science and Technology, Ryukoku University, Seta, Otsu 520-2194, Japan Abstract In this research, nano polyacrylonitrile (PAN) fiber was spun by Cotton Candy Method (CoCaM). CoCaM is the novel method to fabricate a nano fiber. This technique is expected to use in various field, because CoCaM has excellent advantages, for example cost reduction, good productivity and so on. We can find that PAN concentration, air pressure and feeding speed affected diameter of nano fiber. CoCaM can make a preparation of various fiber sizes. The minimum and maximum number average of nano PAN fiber diameter were ranged from macro to nano meters. After carbonizing, the diameter of nano fibers was decreased 16% compared to nano PAN fibers. According to the result of Raman spectrometry, it is revealed the high crystallinity of nano carbon fiber. Introduction Recently, it has been possible to make a preparation of nano fibers in the technology field [1-4]. The diameter of nano fibers is under several hundreds nano meters. They have several excellent properties such as mechanical properties and large surface area. Therefore, nano fibers are expected to apply in various field including energy sector, electronics sector, medical sector and so on. Several methods for fabricating nano fibers were reported by researchers, electrospinning method is one of the most famous methods [5-9]. The electrospinning method can fabricate the nano fibers by dissolved resin in the solution with a high voltage. In the result, it is possible to make the nano fibers to stretch the dissolved resin by electrostatic repulsion. However, the electrospinning method results in large cost because of keeping the high voltage during the produce. Besides, the electrospinning method does not have enough stretching process. Therefore, the nano fibers that are fabricated by electrospinning method are low crystallinity and weak mechanical properties. On the other hands, carbon fibers have gotten a lot of attention recently because they have excellent mechanical properties and use in various fields [10-12]. Several ways to produce carbon fibers are reported. Carbon fibers are typically made from polyacrylonitrile (PAN) [13-14]. Carbonization of PAN fibers has two steps. The first step is called flame-proofing which is heating in an oxygen atmosphere at 200 to 300 ℃. In the second step, PAN is carbonized between 700 and 1800 ℃ in a nitrogen atmosphere. In this research, the novel method that called Cotton Candy Method (CoCaM) is introduced. PAN that is precursor of carbon fiber was solved in Nmethylpyrrolidone (NMP). This solution was blown and stretched by air. After that stretched nano fiber was caught in water. NMP is a good solvent for PAN, whereas water is a poor solvent for PAN. This simple process can fabricate PAN nano fibers. Since the CoCaM does not need a high voltage, this novel method is expected to produce in large volume in a low cost way. For looking at the effect of spinning condition on nano fibers, polymer concentration, air pressure and feeding speed of polymer were varied. After carbonization, Raman spectrometry was carried out in order to evaluate crystallinity of nano carbon fiber [15-16]. Experiment Materials Polyacrylonitrile (PAN, Mw: 150,000) was used, it was manufactured by Sigma-Aldrich Co. LLC., America. N-methyl-2-pyrrolidone (NMP) was used as solvent, which was manufactured by NACALAI TESQUE, INC., Japan. PAN was dissolved in NMP, and the solutions that contained 3%, 5%, 10% and 15% PAN were prepared respectively. Cotton Candy Method Cotton Candy Method was used in this research. Figure 1 shows the schematic of CoCaM machine. Three SPE ANTEC™ Indianapolis 2016 / 508 holes for feeding solution are located above an air outlet. The solution was feeding thorough a routed screw, after that it was blown and stretched by air. The stretched PAN solution was corrected in water and deposited as nano PAN fiber. of nano carbon fiber. From this result, the ratio of the D and G peak intensities (ID/IG) was calculated. Fiber Diameter Determination Diameter of nano fiber was measured by SEM photograph. From these results, fiber diameter distribution was determined. The number average fiber diameter (DN) was defined by the following equation. (1) DN = ∑ Ni Di ∑N i where Ni is number of fiber at the diameter Di Carbonization ! Figure 1. Schematic of CoCaM machine. Carbonization was carried out in two steps. The first step is flame-proofing. The nano PAN fibers were heated room temperature to 270 ℃ with heating rate of 5℃/min, held for an hour under compressed air atmosphere. In second step, carbonizing was carried out. The flame-proofed fibers were heated until 1400 ℃ with heating rate 7 ℃/min. And then held at 1400 ℃ for 10 minutes in nitrogen atmosphere. In this method, 3 processing parameters were revealed. For looking at the effect of PAN concentration in NMP, 4 various contents of PAN solution (3%, 5%, 10% and 15%) were prepared and tested. screw speed for feeding solution was set 30 rpm with air pressure of 0.1 MPa in this test. In addition, the effect of air pressure was studied at 0.05 MPa, 0.2 MPa and 0.4 MPa by using PAN solution of 10%. And screw speed for feeding solution was set 30 rpm. After that, experiment was focused on the effect of feeding screw speed of solutions. The screw for feeding was varied at 5 rpm and 30 rpm. In this experiment, PAN concentration of 10% was used, and Air pressure was set 0.2 MPa. Results and Discussion Mechanism of CoCaM High-Speed Camera PAN was dissolved in NMP and this solution was injected at a constant feed rate though the nozzle. The observation by high-speed camera is shown in Figure 2. PAN solution was stretched by swirled flow of air. The swirl flow could make PAN solution blanched efficiently. The blanched solution was stretched until diameter of that became nano size. Air outlet High-speed camera (PHOTRON LIMITED : model FASTCAM SA4 ) was used for observing mechanism of CoCaM. Branching Scanning Electron Microscope Scanning electron microscope (JEOL: model JSM5200) was conducted to observe configuration of nano fiber. The specimen was mounted on aluminum holder and gold sputtered for 2 minutes prior observation. Raman Spectrometry Raman spectrometer (JASCO Corporation: model RMP-510RS) was used in order to evaluate crystallinity Stretched PAN ! Figure 2. Photograph of stretched PAN solution by High– speed camera SPE ANTEC™ Indianapolis 2016 / 509 Effects of PAN concentration on fiber diameter SEM photographs of nano PAN fibers are presented in Figure 5. Shapes of nano PAN fibers are almost constant and their surfaces are smooth. The diameters of nano fibers are decreased with the increasing of air pressure. SEM photographs of nano PAN fiber that fabricated by different concentration are presented in Figure 3. The diameters of nano fibers are decreased with the reducing of PAN concentration. Moreover, they also reveal inconstant shapes along nano PAN fibers. (a) (e) (f) (b) ! ! (g) ! ! (c) (d) ! Figure 5. SEM observation of nano PAN fiber produced by different magnitude of air pressure (e) 0.05 MPa, (f) 0.2 MPa and (g) 0.4 MPa. ! ! Figure 3. SEM photographs of nano PAN fiber produced by different PAN concentration (a) 3%, (b) 5%, (c) 10% and (d) 15%. The effects of PAN concentration on number average fiber diameter is shown in Figure 4. The minimum and maximum number average fiber diameter are range from 70 nm to 1980 nm. The reducing of PAN content led to the decreasing of number average fiber diameter. It is guessed that PAN content in solution that shaped fiber was reducing. Figure 6 shows the relative of air pressure and number average fiber diameter. The minimum and maximum number average fiber diameter are range from 340 nm to 2090 mm. The increasing of air pressure led the decreasing of number average fiber diameter. This result indicates that high pressure air blow can stretch solution more efficiently than low pressure air blow. ! Figure 6. The effects of air pressure on number average fiber diameter ! Figure 4. The effects of PAN concentration on number average fiber diameter Effects of magnitude of Air pressure on fiber diameter Effects of feeding speed on fiber diameter Figure 7 shows SEM photographs of nano fibers that were fabricated by using5 rpm and 30 rpm feeding speed. The nano fibers fabricated by feeding screw speed of 5 rpm are not smooth. These diameters of nano fibers are decreased with the reducing of rotating screw speed for feeding solution. SPE ANTEC™ Indianapolis 2016 / 510 (h) The comparison between diameter of nano PAN fiber and that of nano carbon fiber is presented in Figure 10. The number average fiber diameter of nano carbon fiber was decreased about 16% by carbonization. (i) ! ! Figure 7. SEM photograph of nano PAN fiber produced by different feeding speed (h) 5 rpm, (i) 30 rpm. The effect of a number average fiber diameter by different feeding speed is shown in Figure 8. The minimum and maximum number average fiber diameter are range from 350 nm to 2230 nm. The decreasing of a number average fiber diameter with the reducing of amount of feed solution is observed. ! Figure 10. The comparison between diameter of nano PAN fiber and that of nano carbon fiber Raman spectrometry ! The Raman spectra of nano carbon fiber is shown in Figure 11. D band has a very shape peak at 1342 cm-1 and FWHM of D peak is 66.95. G band has a small peak at 1573 cm-1 and FWHM of G peak is 23.87. These peaks separate completely. The ratio of the D and G peak intensities (ID/IG) is 0.58. This value indicates high crystallinity of nano carbon fiber. It is guessed that nano fiber fabricated by CoCaM is stretched strongly and polymer chain is aligned. Figure 8. The effects of feeding speed on number average fiber diameter Carbonization The nano PAN fiber at 3% PAN concentration was selected to make nano carbon fiber, because they were the finest nano PAN fibers. As shown in figure 9, SEM photograph exhibits the remained nano fibers from carbonization process. G peak D peak ! ! Figure 11. Raman spectra of nano carbon fiber Figure 9. SEM observation of nano carbon fiber Conclusions SPE ANTEC™ Indianapolis 2016 / 511 In this research, we can find that nano polyacrylonitrile (PAN) fibers were spun by Cotton Candy Method (CoCaM) in several processing conditions. After spinning nano PAN fibers, carbonization of those fibers were carried out. Under the observation of High-speed camera, it is become apparent mechanism of CoCaM. PAN solution was stretched by swirled flow of air. The swirl flow could make PAN solution blanched efficiently. The changing of PAN content, air pressure and feeding speed have an effect on diameter of nano fibers. The diameters of nano fibers are decreased with the reducing of PAN concentration. The diameters of nano fibers are decreased with the increasing of air pressure. The diameters of nano fibers are decreased with the reducing of amount of feed solution. After carbonizing, shapes of nano fibers were remained. The number average fiber diameter of nano carbon fiber decreased about 16% by carbonization. Raman spectrometry of nano carbon fiber by CoCaM shows high crystallinity. The ratio of the D and G band intensities (ID/IG) of carbon nano fiber is 0.58. It is guessed that nano fibers by CoCaM are stretched strongly and polymer chain is aligned. CoCaM is a new process for fabricating nano fibers without high voltage and ion dope. This technology provides us high-volume production of nano fibers in a low-cost way. 12. Y. Maeda, The Recent Trends of Carbon Fiber, (2007) 13. H. ASANO, E. NAKADA and Y. SATO, Study on Strength improvement of Activated Nano Carbon Fiber Sheet (2012). 14. J. Jang, J. Bae and E. Park, Polyacrylonitrile Nanofibers: Advanced Functional Materials, 16, 11, 1400 (2006) 15. F. C. Tai1, S. C. Lee1, C. H. Wei and S. L. Tyan, Materials Transactions, Vol. 47, No. 7 1847 (2006). 16. L. G. Cançado,a K. Takai, T. Enoki, M. Endo, Y. A. Kim, H. Mizusaki, A. Jorio, L. N. Coelho, R. Magalhães-Paniago, and M. A. Pimenta, APPLIED PHYSICS LETTERS 88, 163106 (2006) References 1. M. Endo and S. Iijima, Handbook of nano carbon (2011) 2. Y. Suda, H. Tanoue and H. Takikawa, J. Plasma Fusion Res. 88, 11, 629(2012) 3. N. A. Jarrah, J. G. V Ommen and L. Lefferts, Journal of Materials Chemistry 14, 1590 (2014) 4. T. L i n , N A N O F I B E R S – P R O D U C T I O N , PROPERTIES AND FUNCTIONAL APPLICATIONS (2011). 5. J. J. Ge, H. Hou, Q. Li, M. J. Graham, A. Greiner, D. H. Reneker, F. W. Harris and S. Z. D. Cheng, JOUNAL OF THE AMERICAN CHEMICAL SOCIETY, 126, 48, 15754 (2004) 6. M. Panapoy, A. Dankeaw and B. Ksapabutr, Thammasat International Journal of Science and Technology, 13 (2008) 7. S. Y. Gu, J. Ren and G. J. Vancso, European Polymer Journal, 41, 11, 2559 (2005) 8. M. H. Zhang, Y. Z. Zhang, M. kotaki, S. Ramakrishna, Composites Science and Technology, 63, 15, 2223 (2003) 9. K. Watanabe, T. Nakamura, B. S. Kim and I. S. Kim, Polymer Bulletin, 67, 2025 (2011) 10. F. Itani, Journal of the Japan Society for Composite Materials, 33, 5, 178, (2007) 11. K. Morita, Carbon fiber theory and application, (1984) SPE ANTEC™ Indianapolis 2016 / 512
© Copyright 2026 Paperzz