Poster Session, Thursday, June 17Theme F686 - N1123Undesired Phase Formations Between Ba 0.5 Sr 0.5 Co 0.8 Fe 0.2 O 3-δ Cathode and La 0.9 Sr 0.1 Ga 0.8 Mg 0.2 O 2.85Electrolyte for SOFCsYeliz EKINCI 1 , Ridvan DEMIRYUREK 2* , Omer KARAKOC 2* , Shalima SHAWUTI 2 , C<strong>in</strong>ar ONCEL 2 and M. Ali GULGUN 21 Faculty of Chemical and Metallurgical Eng<strong>in</strong>eer<strong>in</strong>g, Istanbul Technical University, Istanbul 34469, Turkey2 Faculty of Eng<strong>in</strong>eer<strong>in</strong>g and Natural Sciences, Sabanci University, Istanbul 34956, TurkeyAbstract Ba 0.5 Sr 0.5 Co 0.8 Fe 0.2 O 3-δ (BSCF) is promis<strong>in</strong>g material as a cathode for La 0.9 Sr 0.1 Ga 0.8 Mg 0.2 O 2.85 (LSGM) based SOFCs. For this aim,BSCF-LSGM powders were characterized by the XRD, SEM and EDS techniques to observe the formation of undesired phases <strong>in</strong> thetemperature range of 700-1100 °C. Formation of new phases began around 900 °C. No new phases were observed below this temperature.SrLaGa 3 O 7 , BaLaGaO 4 and Ba 6 La 2 Co 4 O 15 could be undesired phases which were strongly observed at 1100 °C.The ma<strong>in</strong> obstacle <strong>in</strong> front of SOFC’s commercializationis their high operat<strong>in</strong>g temperatures [1]. Efforts to reduce theoperat<strong>in</strong>g temperature br<strong>in</strong>gs along some problems with them.There is a substantial <strong>in</strong>crease <strong>in</strong> electrochemical resistance ofthe fuel cell components (anode, cathode and electrolyte) andan <strong>in</strong>crease of electrode polarization resistance [2]. To tacklethese problems, novel materials has been under an <strong>in</strong>tensestudies. Ba 0.5 Sr 0.5 Co 0.8 Fe 0.2 O 3−δ (BSCF) cathode andLa 0.9 Sr 0.1 Ga 0.8 Mg 0.2 O 2.85 (LSGM) electrolyte materialcomb<strong>in</strong>ation offers promis<strong>in</strong>g results. LSGM is preferredbecause of its high oxygen ion conductivity, 10 -1 S cm -1 [3] at800 °C and high oxygen diffusion rate. The electronicconductivity pattern over a wide range of oxygen partialpressures (10 − 20 to 1 atm) can be assumed negligible at<strong>in</strong>termediate operat<strong>in</strong>g temperatures [3]. BSCF is a mixedoxygen ionic and electronic conduct<strong>in</strong>g oxide <strong>in</strong> the latticeform of perovskite [2]. High activity to reduce the oxygenelectrochemically and high oxygen diffusion rate at 773-873°C makes BSCF worthy of <strong>in</strong>vestigation [3]. However use ofBSCF cathode and LSGM electrolyte together may causeformation of some undesired phases. These undesired phasescould decrease the efficiency of the whole system.In this <strong>in</strong>vestigation, the temperature range at whichundesired reactions between the cathode candidate and theLSGM electrolyte take place and the phases that are formedwere studied. BSCF used <strong>in</strong> this study was synthesized bycomb<strong>in</strong>ed EDTA-citrate (EC) method [4]. The temperature ofthe formation of reaction products was determ<strong>in</strong>ed by XRD.LSGM and BSCF powders are mixed <strong>in</strong> the ratio of 1:1. XRDmeasurements are done on the powders heat treated at roomtemperature (RT), 700 C, 800 C, 900 C, 1000 C, and 1100C (Figure 1). Formation of new phases began around 900 C.No new phases were observed below this temperature. Thephase that was strongly consumed <strong>in</strong> the reactions above 1100°C was BSCF. The disappearance of XRD peaks belong<strong>in</strong>g toBSCF phase can be observed <strong>in</strong> Figure 1.The new phases that form as a result of the reactions betweenthe cathode and electrolyte are suspected to be SrLaGa 3 O 7,BaLaGaO 4 and Ba 6 La 2 Co 4 O 15 .Figure 2 shows the secondary electron and back scatteredelectron images of a particle that shows reacted as well asorig<strong>in</strong>al powder regions. EDS analyses taken from regionswith different BSE contrast <strong>in</strong> Figure 2 confirmed theassignments of the phases that appear <strong>in</strong> these reactions. EDSresults also <strong>in</strong>dicated that extensive solid solution <strong>in</strong> thesystem is possible. This could open a whole new series ofmixed oxides that are suitable for SOFC applications.Figure 2. SEM micrographs of mixture of BSCF-LSGM powders at1100 °C (a) the secondary electron (b) the back scattered electron*Present<strong>in</strong>g authors: demiryurek@su.sabanciuniv.edu,okarakoc@su.sabanciuniv.edu[1] Liu, B., Zhang, Y., and Zhang, L., 2008. Journal of PowerSources. Volume 175, Issue 1, Pages 189-195[2] Zhou, W., Ran, R., and Shao, Z., 2009. Journal of Power Sources,Volume 192, Issue 2, Pages 231-246[3] J. Peña-Martíneza, D. Marrero-Lópezb, J.C. Ruiz-Moralesb, B.E.Buergler, P. Núñez and L.J. Gauckler, 2006. Solid State Ionics,Volume 177, Issue 19-25, Pages 2143-2147[4] Lee, S., Lim, Y., Lee, E., Hwang, H., and Moon, J, 2005. Journalof Power Sources, Volume 157, Pages 848-854(a)(b)Figure 1. The XRD patterns of mixture of BSCF-LSGM powders6th Nanoscience and Nanotechnology Conference, zmir, 2010 770
Poster Session, Thursday, June 17 Theme F686 - N1123Enhanced Photocatalytic Activity Of Dye-Sensitized SolarCells With Optimized CathodeBerk H. Giray a , Hermann Tempel b,c , Sayg<strong>in</strong> Aras c , Özlem Soydas c , Jörg J.Schneider b , and Deniz Üner c,*a Aselsan Inc., 06172, Ankara / TURKEYb Eduard-Z<strong>in</strong>tl Institut Technische Universität Darmstadt, Petersenstrasse 18 64287 Darmstadt, GERMANYc Middle East Technical University, Chemical Eng<strong>in</strong>eer<strong>in</strong>g Department, 06531, Ankara / TURKEY*uner@metu.edu.trAbstract. In this study the effect of CNT modified TiO 2 th<strong>in</strong> films on the performance of Dye Sensitized SolarCells (DSSC) is studied. Furthermore, the effect of the thermal decomposition temperature of Pt layer on thecathode surface was also <strong>in</strong>vestigated. The CNT load<strong>in</strong>gs and Pt decomposition temperatures were optimized forthe efficiencies of the DSSCs.Keywords: dye sensitized solar cells, carbon nanotubes, Pt load<strong>in</strong>gs, metal support <strong>in</strong>teraction.PACS: 81.40.Tv - Optical and dielectric properties related to treatment conditions:http://www.aip.org/pacs/<strong>in</strong>dex.htmlINTRODUCTIONS<strong>in</strong>ce the <strong>in</strong>troduction of DSSC from Grätzel andO’Regan [1] , numerous studies have been done tooptimize the work<strong>in</strong>g electrode. But still theefficiencies are limited to less than 10-15% [2] . Themajority of the studies focus on the anode side of theDSSCs. However, there is also room for improvement<strong>in</strong> the catalysis go<strong>in</strong>g on at the Pt nanoparticles overthe cathode surface.EXPERIMENTALPt layer was coated by brushcoat<strong>in</strong>g of platisol(Solaronix Switzerland). After coat<strong>in</strong>g the plat<strong>in</strong>umprecursor was decomposed by heat treatment at 400°Cfor 5 m<strong>in</strong>. Afterwards s<strong>in</strong>ter<strong>in</strong>g at temperatures from400°C to 550°C were applied. The work<strong>in</strong>g electrode(anode) was prepared by doctor blade technique. Theprecursor solution was Ti-Nanoxide T20 (Solaronix)was the choice of anatase. It is a paste conta<strong>in</strong><strong>in</strong>g 11weight % anatase with uniform particle diameter of 20nm.CNTs were <strong>in</strong>corporated <strong>in</strong>to the work<strong>in</strong>g electrodeTiO 2 by stir<strong>in</strong>g ethanol, anatase nanopowder,tetratitaniumisopropoxide, nitric acid, polyethyleneglycoland pluronic at 50°C for 20h. This sol wasapplied onto the FTO glass slides by sp<strong>in</strong>coat<strong>in</strong>gtechnique [3] .RESULTS AND DISCUSSIONThe amount of Ru-Dye [Solaronix Ru-535]adsorbed <strong>in</strong>creased upon <strong>in</strong>corporation of activatedcarbon on the anode. But, it should be rememberedthat a larger amount of dye not always leads to highercurrent <strong>in</strong> the DSSC. Figure 1 shows the TiO 2 layerwith <strong>in</strong>corporated CNTs.The effects of the different s<strong>in</strong>ter<strong>in</strong>g parameters on thecathode surface morphology were reported <strong>in</strong> terms ofthe effect on the cell efficiency and the fill factor <strong>in</strong>Table 1. It is seen that the catalytic I - /I 3 - reactions atthe cathode side is <strong>in</strong>fluenced by the Pt particle sizes.Further characterization is <strong>in</strong> progress.FIGURE 1. SEM image of TiO 2 film with<strong>in</strong>corporated CNTs.TABLE 1. Effect of different anneal<strong>in</strong>g conditions onthe cell performance [4]particles size P FF ηT( o C) (nm)(mW) (%)none 89 24,50 0.454 2.36450 83 25,80 0.466 2.48500 69 29,60 0.471 2.85550 67 30,00 0.474 2.89ACKNOWLEDGMENTSF<strong>in</strong>ancial support of BMBF Germany andTUBITAK (107M447) Inten-C jo<strong>in</strong>t program andTUBITAK (108M631) is acknowledged. METUCentral laboratories and the Metallurgical andMaterials Eng<strong>in</strong>eer<strong>in</strong>g Department are k<strong>in</strong>dlyacknowledged for the SEM measurements.REFERENCES1. Grätzel and O’Regan, Nature, 353, 1991, 737.2. Hodes G. Electrochemistry of nanomaterials, VCH-Wiley, We<strong>in</strong>heim, 2000.3. H. Itai, H. et al. Chemistry Letters,No. 9, 37, 2008, 940.4. H. B. Giray M.S Thesis, 2010, METU, Ankara.6th Nanoscience and Nanotechnology Conference, zmir, 2010 1
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