| 研究生: |
蔡宗承 Tsai, Tsung-Chen |
|---|---|
| 論文名稱: |
使用奈米膜在微流體與奈米流體系統之微型可逆電透析的能量產生 Power Generation by Reverse Electrodialysis in Nanopore Membranes from a Microfluidic and Nanofluidic System |
| 指導教授: |
楊瑞珍
Yang, Ruey-Jen |
| 學位類別: |
碩士 Master |
| 系所名稱: |
工學院 - 工程科學系 Department of Engineering Science |
| 論文出版年: | 2016 |
| 畢業學年度: | 104 |
| 語文別: | 英文 |
| 論文頁數: | 51 |
| 中文關鍵詞: | 可逆電透析,鹽分梯度能源 、吉布斯自由能 、納菲翁薄膜 、能源轉換 |
| 外文關鍵詞: | Reverse electrodialysis, Salinity gradient power, Gibbs free energy, Nafion membrane, Energy conversion |
| 相關次數: | 點閱:94 下載:4 |
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本研究利用微機電製程技術,使用新方法去製作直通管式的通道(1 mm, 2 mm, 3 mm)並且注入具有陽離子選擇性的納菲翁(Nafion)溶液,等待乾燥而形成薄膜,利用可逆電透析原理並在通道兩邊儲存槽放置不同濃度的氯化鉀(KCl)溶液。不同鹽度梯度氯化鉀溶液(CL:1 mM CH:10 mM,100 mM,1000 mM,2000 mM)混合所產生的吉布森自由能轉換成電能。我們量測納菲翁(Nafion)膜的電壓-電流曲線,並可從此獲得擴散電壓、離子遷移數、功率值與效率。並由實驗得到最佳的擴散電位為152 mV,擴散電流為249 nA,最大功率為755 mW/m2,本實驗的最佳效率為31%。根據歐姆定律,在定電壓情況下,當管道長度縮短時阻值降低然而相對提升電流值,當電解液濃度梯度增加時,也會提高擴散電位,其中擴散電位關係到電場強度大小,電場強度越大所造成在遷移陽離子的阻力,而陽離子遷移路徑是由高濃度往低濃度方向,因此上述使整體電流值並無隨著濃度梯度提高而增大
In this thesis, we propose the fabrication of an energy conversion microchip using a standard micro-electromechanical technique. Moreover, this new device uses a microfluidic channel (Length:1 mm, 2 mm, 3 mm) with injected Nafion solution, and then dried to become a cation-selective membrane between two KCl solutions with various concentration combinations (CL:1 mM CH:10 mM,100 mM,1000 mM,2000 mM) by reverse electrodialysis. The Gibbs free energy of mixing from a salinity gradient can be converted into electrical energy by using a selective membrane. We measured the current-potential characteristics of the Nafion membrane so that the diffusion potential, transference number, power values, and efficiency can be obtained. The highest measured diffusion potential, short-circuit current, and power density are 152 mV, 249 nA, and 755 mW/m2, respectively, while the best efficiency obtained in this study was 31 %. According to Ohm’s Law, and when the voltage is constant, the highest current occurs when the channel length is the shortest. Moreover, a longer channel length causes more resistance, so the produced power is smaller. If the electrolyte concentration ratios are increased, the diffusion potential will be enhanced. The electrical field is related to the diffusion potential, and it produced a barrier to the cation migration from high concentration to low concentration. Accordingly, the short circuit current was not enhanced at a high concentration ratio.
[1] L. Kazmerski, Renewable & sustainable energy reviews. U.K: Oxford, 1997.
[2] G. L. Wick, "Power from salinity gradient," Energy, vol. 3, pp. 95-100, 1978.
[3] H. C. Yeh, C. C. Chang, and R. J. Yang, "Reverse electrodialysis in conical-shaped nanopores: salinity gradient-driven power generation," RSC Advanves, vol. 4, pp. 2705-2714, 2014.
[4] S. Lee, H. Kim, and D. K. Kim, "Power generation from concentration gradient by reverse electrodialysis in dense silica membranes for microfluidic and nanofluidic systems," Energies, vol. 9, pp. 49, 2016.
[5] A. Demirbaş, "Biomass resource facilities and biomass conversion processing for fuels and chemicals," Energy Conversion and Management, vol. 42, pp. 1357-1378, 2001.
[6] T. Ackermann, "Wind energy technology and current status a review," Renewable and Sustainable Energy Reviews, vol. 4, pp. 315-374, 2000.
[7] O. Mahian, A. Kianifar, S. A. Kalogirou, I. Pop, and S. Wongwises, "A review of the applications of nanofluids in solar energy," International Journal of Heat and Mass Transfer, vol. 57, pp. 582-594, 2013.
[8] D. K. Kim, C. Duan, Y. F. Chen, and A. Majumdar, "Power generation from concentration gradient by reverse electrodialysis in ion-selective nanochannels," Microfluidics and Nanofluidics, vol. 9, pp. 1215-1224, 2010.
[9] B. D. Kang, H. J. Kim, M. G. Lee, and D. K. Kim, "Numerical study on energy harvesting from concentration gradient by reverse electrodialysis in anodic alumina nanopores," Energy, vol. 86, pp. 525-538, 2015.
[10] C. C. Chang and R. J. Yang, "Electrokinetic energy conversion in micrometer-length nanofluidic channels," Microfluidics and Nanofluidics, vol. 9, pp. 225-241, 2009.
[11] C. C. Chang and R. J. Yang, "Electrokinetic energy conversion efficiency in ion-selective nanopores," Applied Physics Letters, vol. 99, pp. 083102, 2011.
[12] J. W. Post, Blue Energy: electricity production from salinity gradients by reverse electrodialysis. Socio-Economic and Natural Sciences of the Environment, 2009.
[13] J. N. Weinstein and F. B. Leitz, "Electric power from differences in salinity: the dialytic battery," Science, vol. 191, pp. 557-559, 1976.
[14] J. D. Isaacs and R. J. Seymour, "The ocean as a power resource," International Journal of Environmental Studies, vol. 4, pp. 201-205, 1973.
[15] F. Suda, T. Matsuo, and D. Ushioda, "Transient changes in the power output from the concentration difference cell (dialytic battery) between seawater and river water," Energy, vol. 32, pp. 165-173, 2007.
[16] J. Veerman, M. Saakes, S. Metz, and G. Harmsen, "Reverse electrodialysis: performance of a stack with 50 cells on the mixing of sea and river water," Journal of Membrane Science, vol. 327, pp. 136-144, 2009.
[17] J. C. Eijkel and A. Van Den Berg, "Nanofluidics: what is it and what can we expect from it?," Microfluidics and Nanofluidics, vol. 1, pp. 249-267, 2005.
[18] G. M. Whitesides, "The origins and the future of microfluidics," Nature, vol. 442, pp. 368-373, 2006.
[19] A. Author, "Energy conversion in microsystems: is there a role for micro/nanofluidics?," Lab on a Chip, vol. 7, pp. 1234-1237, 2007.
[20] W. Guo, L. Cao, J. Xia, F. Q. Nie, W. Ma, J. Xue, et al., "Energy harvesting with single‐ion‐selective nanopores: A concentration‐gradient‐driven nanofluidic power source," Advanced Functional Materials, vol. 20, pp. 1339-1344, 2010.
[21] V. Tandon, S. K. Bhagavatula, W. C. Nelson, and B. J. Kirby, "Zeta potential and electroosmotic mobility in microfluidic devices fabricated from hydrophobic polymers: 1. The origins of charge," Electrophoresis, vol. 29, pp. 1092-1101, 2008.
[22] L. Cao, W. Guo, W. Ma, L. Wang, F. Xia, S. Wang, et al., "Towards understanding the nanofluidic reverse electrodialysis system: well matched charge selectivity and ionic composition," Energy & Environmental Science, vol. 4, pp. 2259-2266, 2011.
[23] J. Kim, S. J. Kim, and D. K. Kim, "Energy harvesting from salinity gradient by reverse electrodialysis with anodic alumina nanopores," Energy, vol. 51, pp. 413-421, 2013.
[24] J. Koryta, J. Dvorak, and L. Kavan, Principles of electrochemistry. New York : Wiley, 1993.
[25] M. C. Gilstrap, "Renewable electricity from salinity gradients using reverse electrodialysis," Scholarly Materials and Research at Tech, 2013.
[26] M. G. Kaifer. A. Kaifer, Supramolecular Electrochemistry. New York : Wiley-VCH, 1999.
[27] A. J. Bard and L. R. Faulkner, Fundamentals and applications. Electrochemical Methods, 2nd ed.; Wiley: New York, 2001.
[28] R. J. Hunter, Zeta potential in colloid science: principles and applications vol. 2: Academic press, 2013.
[29] R. F. Probstein, Physicochemical hydrodynamics: an introduction: John Wiley & Sons, 2005.
[30] J. Veerman, M. Saakes, S. J. Metz, and G. Harmsen, "Reverse electrodialysis: evaluation of suitable electrode systems," Journal of Applied Electrochemistry, vol. 40, pp. 1461-1474, 2010.
[31] K. A. Mauritz and R. B. Moore, "State of understanding of Nafion," Chemical Reviews, vol. 104, pp. 4535-4586, 2004.
[32] A. Sahu, S. Pitchumani, P. Sridhar, and A. Shukla, "Nafion and modified-Nafion membranes for polymer electrolyte fuel cells: An overview," Bulletin of Materials Science, vol. 32, pp. 285-294, 2009.
[33] NANO SU-8 2000 Negative Tone Photoresist Formulations 2002-2025.
[34] NANO SU-8 2000 Negative Tone Photoresist Formulations 2015.
[35] J. Yoon, Y. Cho, S. Han, C. S. Lim, J. H. Lee, and S. Chung, "Microfluidic in-reservoir pre-concentration using a buffer drain technique," Lab on a Chip, vol. 14, pp. 2778-2782, 2014.
[36] S. Bhattacharya, A. Datta, J. M. Berg, and S. Gangopadhyay, "Studies on surface wettability of poly (dimethyl) siloxane (PDMS) and glass under oxygen-plasma treatment and correlation with bond strength," Journal of Microelectromechanical Systems, vol. 14, pp. 590-597, 2005.
[37] J. H. Lee, Y.-A. Song, and J. Han, "Multiplexed proteomic sample preconcentration device using surface-patterned ion-selective membrane," Lab on a Chip, vol. 8, pp. 596-601, 2008.
[38] N. Lakshminarayanaiah, "Transport phenomena in artificial membranes," Chemical Reviews, vol. 65, pp. 491-565, 1965.