The 9th overseas Symposium on sturdy Oxide gasoline Cells: fabrics, technology, and know-how was once held in January 2012 as a part of the thirty sixth foreign convention on complicated Ceramics and Composites (ICACC). This symposium supplied a global discussion board for scientists, engineers, and technologists from worldwide to provide and speak about the newest advances in sturdy oxide gas cells. This factor good points fourteen papers chosen from the symposium, delivering readers a vast landscape of the present prestige of reliable oxide gasoline cells know-how, in addition to rising matters and destiny instructions within the field.
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Additional resources for Advances in Solid Oxide Fuel Cells VIII
H. Etsell, P. Sarkar, Dip coating fabrication process for micro-tubular SOFCs, Solid State Ionics, 192 (2011), 372. M. Sammes, Y. Du, R. Bove, Design and fabrication of a 100W anode supported micro-tubular SOFC stack, Journal of Power Sources, 145 (2005), 428-434. 3 K. Kendall, Progress in Microtubular Solid Oxide Fuel Cells, Int. J. Appl. Ceram. Technoi, 7 , (2010), 1. P. G. Love, L. Apateanu, Effect of contact between electrode and current collector on the performance of solid oxide fuel cells, Solid State Ionics, 160 (2003,) 15.
Flow rates of gases were controlled between 40 and 100 mL min"1 at one atmosphere pressure. The performance analysis of the fuel cells was carried out using potentistat/galvanostat (Autolab, PGSTAT 30). The measurements were performed from 450 °C to 650 °C with humidified hydrogen (2% H 2 0) as fuel and air as oxidant. Figure 9 compares the I-V curves and power density of single cell at three temperatures 450, 550 and 650 °C respectively. The power density increased with increasing temperature while OCV remains the same and a maximum power density of 380 mWcm 2 is obtained at 650 °C.
E. 02 dpb%. In this case the ascending and descending ramps are almost superimposed and this means that the microstructure of suspension is far not affected by the shear history and stable over the time involved for the measurement. For +95 and especially for +57 suspension the hysteresis loops are quite evident and the suspensions microstructure depends on shearing. For both suspensions, powder agglomeration occurs along the descending ramp and viscosity is increased. 16 On the other hand irreversible changes of suspension microstructure can be related to evaporation of suspension solvent.