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![]() New Journal of Glass and Ceramics, 2011, 1, 58-62 doi:10.4236/njgc.2011 .12007 Published Online July 2011 (http://www.SciRP.org/journal/njgc) Copyright © 2011 SciRes. NJGC Synthesis and Characterization of La0.75Sr0.25Cr0.5Mn0.5O3-δ Nanoparticles Using a Combustion Method f or Solid Oxide Fuel Cells V. S. Reddy Channu1, Ru d ol f Ho lz e1, E dwin H. Walker Jr.2, Rajamohan R. Kalluru3 1Institut für Chemie, AG Elektrochemie, Technische Universität Chemnitz, Chemnitz, German y; 2Department of Chemistry, South- ern University and A&M College, Baton Rouge, USA; 3KITE College of Professional Engineering Sciences, Jawaharlal Nehru Technological University of Hyderabad, Shabad, India. Email: [email protected] Received April 11th, 2011; revised May 9th, 2011; accepted May 16th, 2011. ABSTRACT La0.75Sr0.25Cr0.5Mn 0. 5O3-δ (LSCM) perovskite nanoparticles for use as anode material in intermediate temperature solid oxide fu el cells (IT-SOFCs) w e re syn th esi zed usi ng 3,3’,3”-nitrilotripropio nic a cid (NTP), citric acid and oxalic acid as carriers via a combustion method. The influence of the carrier on phase and morphology of the obtained pristine prod- ucts was characterized using X-ray diffraction (XRD), thermal gravimetric analysis (TGA), and scanning electron mi- croscopy (SEM). XRD results showed, that the LSCM had rhombohedral symmetry with R-3c space group; a single phase LSCM perovskite formed after calcination of fired gel at 1200˚C for 7 h. Scanning electron microscopy analysis of the pristine powders showed spherical shape and particle sizes in the range of 50 - 500 nm.. Keywords: Nanoparticles, Combustion method, Morphology, Carriers 1. Introduction A fuel cell is an electrochemical device that converts chemical energy of fuels (hydrogen, methane, butane or even gasoline and diesel) into electrical energy by ex- ploiting the natural tendency of oxygen and hydrogen to react. Fuel cells are simple devices co nta ini ng no mo vin g parts and only four functional components namely ca- thode, electrolyte, anode and interconnect. Solid oxide fuel cells (SOFCs) are considered to be among the most versatile power production facilities. Their unique cha- racteristics include extre me efficiency, sig nificant energy conversion rate with a wide range of fuels and pollu- tion-free operation. On the other hand high operating temperature (about 1000˚C) of the SOFC results in pro b- lems including difficult sealing between cells with flat plate configurations and thermal expansion mismatches between components. In addition, the high operating temperature places rigorous constraints on materials se- lection and results in difficult fab rication proc e sses [1]. Recently, perovskite based conducting oxides, such as substituted lanthanum chromites or lanthanum manga- nates and strontium titanates, received great attention as alternative anode materials for solid oxide fuel cells [2]. Particularly, (La0.75 Sr 0.25)1-xCr0.5 Mn 0.5O3−δ perovskite phase (LS C M) has been considered as a capable anode material for SOFCs d ue to its electro catal ytic/catalytic acti vity for oxidation of methane fuel in the absence of steam, re- duced carbon deposition, and high durability a gainst sul- fur poisoning and good electrical properties [3,4]. Pre- dominantly, this composition of LSCM has shown good stability in fuels and in air, and has good resistance to- wards carbon deposition and low polarization resistance when used with hydrocarbon fuels [5]. LSCM can also be used as a cathode, thus facilitating fuel cells with a symmetrical structure (LSCM/electrolyte/LSCM) [6,7]. Up till now, various chemical methods were reported in the literature for the synthesis of LSCM powders, for example, glycine nitrate method [3], EDTA (ethylenedia minetetraacetic acid) chelating method [8,9], combustion synthesis [7,10], solid-state reactio n [4,6,11-15], gel-casting [16,17] and co-prec ipitation method [18 ]. The so lid-state ![]() Synthesis and Characterization of La0.75Sr0.25Cr0.5Mn0.5O3-δ Nanoparticles Using a combustion M ethod for Solid Oxide Fuel Cells Copyright © 2011 SciRes. NJGC 59 method has some disadvantag es suc h as high temperature (above 1300˚C) and long duration of synthesis of LSCM and non-homogeneity in pa rticle size and low purity [19]. However, to synthesize homogeneous fine particles of pure phase LSCM powders requires low temperature and short duration of synthesis. The solution combustion method is suitable to synthesize nanosize LSCM particles with good homogeneity [20]. The present work reports on the synthesis of nanostructured La0.75Sr 0. 25 Cr0.5Mn0.5 O3−δ (LSCM) perovskite by a combustion method using 3,3’,3”-nitrilotripr opionic ac id, oxalic acid and citric acid as carriers. 2. Experimental Nanostructured La0.75Sr0. 25Cr0.5Mn0.5O3−δ (LSCM) pero- vskite anode material was synthesized by a combustion technique. Three batches of LSCM solutions are pre- pared with stoichiometric amounts of lanthanum nitrate (La(NO3)3·6H2O), strontium nitrate (Sr(NO3)2), chro- mium nitrate (Cr(NO3)3·9H2O) and manganese nitrate (Mn(NO3)2) in distilled water under constant stirring. First, a stoichiometric amount of citric acid (C6H8O7 H2O) and 15 ml ethyle ne glycol, second, oxalic acid and 15 ml ethylene glycol, and 3,3’,3”-nitrilotripro pionic acid and 15 ml et h yle ne gl yc ol whi c h ar e che latin g a ge nt s a nd fuel, were also dissolved in LSCM solution. The stoi- chiometric ratio of carriers to nitrates was 2 [21]. A gel was formed with continuous stirring and mild heating at 120˚C. The gel was dried at room temperature for over- night a nd the n heated at 350˚C for 30 min. The resulting powders were ground in an agate mortar and heated in air at 1000˚C for 7 h. F inal l y, the ground product was heated at 1200˚C for 7 h in air. Crystallographic information of the samples was ob- tained using an X-ray powder diffractometer (D8 Ad- vanced Brucker) with graphite monochromatized Cu Kα radiation (λ = 1.54187 Å). Diffraction data were col- lected over the 2θ range of 15˚ to 80˚. The morphologies of the resulting products were characterized using a scanning electron microscope (SEM, JEOL JSM 6390). For the TGA measurements a TA 600, operating in dy- namic mode (heating rate = 10˚C/min) , was employed. 3. Results and Discussion Phase purity and crystallographic information of the synthesized La0.75Sr0.25Cr0.5Mn0.5O3-δperovskite nanopar- ticles were characterized using powder X-ray dif fraction. The XRD patterns of LSCM perovskite nanoparticles are shown in Figure 1. All diffraction patterns of La0.75Sr0. 25Cr0.5Mn0.5O3-δ perovskite nanoparticles show characteristic peaks of the perovskite phase. The XRD patterns are in good agreement with the standard data for rhombohedral symmetry with a = 5.4736 Å, b = 5.4736 Å, c = 13.2898 Å and R-3c space group (JCPDS # 01-070-8673). No impurity phases were observed pre- sumably because in the solid-state reaction the pure phase of La0.75Sr0.25Cr0.5Mn0.5O3-δ (LSCM ) perovskite was formed at 1200˚C [21]. The crystallite size of the LSCM nanoparticles was calculated using Debye-Scherrer formula at (110) plane. The size of the LSCM-particles prepared NTP-assisted is 57.65 nm, with citric acid and oxalic acid the value is 68.63 nm. In the synthesis of La0.75Sr 0. 25Cr0.5Mn0.5O3-δ (LSCM) perovskite nanoparticles the carriers (NTP, oxalic acid and c itri c aci d) he lp i n ob tai ning a ho moge neous mi xtur e of the cations in a solution through forming metal com- plexes, they also help in the reduction of nitrates in a combustion process, releasing a large amount of heat. This is sho wn by an exothermic peak at 377˚C on a DS C curve (Figure 2). During the solid-state reduction process, metal cations and oxygen anions stay in the react and mixture during the formation of perovskite phase in t his combustion process. The large heat released during combustion might be of the help to overcome the lattice energy, which is required for the formation of the perovskite phase, and also the completion of the nu- cleation by the rearrangement of atoms by short distance diffusion. The fast combustion process might not be of help for the diffusion of atoms far from each other and hence the particle size of LSCM powder remained in the nanometer range [22]. Thermogravimetric analysis and differential scanning calorimetry (TGA-DSC) curves with NTP-assisted LSCM dried as a gel at 120˚C are sho wn in Figure 2. The weight losses happen in three steps. The total weight loss 20 30 40 50 60 7080 La 0.75 Sr 0.25 Cr 0.5 Mn 0.5 O 3-δ (NTP +EG at 1200 O C) 2θ/° 57.65 nm 68.63 nm La 0.75 Sr 0.25 Cr 0.5 Mn 0.5 O 3-δ (OA+EG at 1200 O C) 68.63 nm La 0.75 Sr 0.25 Cr 0.5 Mn 0.5 O 3-δ (CA+EG at 1200 O C) Intensity/s -1 (214) (024) (006) (202) (113) (104) (110) (JCPDS # 01-070-8673) (012) Figure 1. XRD patterns of La0.75Sr0.25Cr0.5Mn0.5O3-δ (LSCM) perovskite phase nanopa rt icles. ![]() Synthesis and Characterization of La0.75Sr0.25Cr0.5Mn0.5O3-δ Nanopar ticles Using a Combustion Method for Solid Oxide Fuel Cells Copyright © 2011 SciRes. NJGC 60 0200 400 600 800100012001400 3 4 5 6 LaSrCrMnO 3 +NTP 0.5mg 0.33mg TGA DSC Temperatur e/ O C W eight loss/mg 1.25 mg -300 -200 -100 0 100 200 Heat flow (mW ) Figure 2. TGA-DSC curves of La0.75Sr0.25Cr0.5Mn0.5O3-δ (LSCM) perovskite g el precursor dried at 120˚C. was 2.1 mg from room temperature to 1300˚C. The first weight loss is 0.33 mg in the temperature range 22˚C - 236˚C; this can be attributed to evaporation of water from the layers of LSCM. The second weight loss is 1.25 mg in the tempera ture ra nge 236˚C - 383˚C and the third weight loss is 0.5 mg in the temperature range 383˚C - 837˚C. The second and third weight losses are attributed to decomposition of the carrier (NTP) and evaporation of structurally bounded water. The peaks located at about 295˚C and 377˚C are exothermic on the DSC curve due to decomposition of nitrates and organic matter and cor- respond to the second weight loss of 1.25 mg from about 236˚C to 400˚C as observed in the TGA curve. To observe thermal effects above 350˚C, different carrier-assisted LSCM samples were fired at 350˚C for 1 h. F igure 3 shows T GA-DT A cur ves of t he di ffere nt c ar- rier’s assisted LSCM samples. The total weight loss was 0.97 mg in NTP assisted LSCM, 0.39 mg in oxalic acid assisted LSCM, and 0.77 mg in citric acid assisted LSCM from room temperature to 1300˚C. The first weight loss is 0.32 mg in NTP assisted LSCM in the temperature range 30˚C - 490˚C, whereas the first weight loss is 0.2 mg in the oxalic acid used LSCM in range 30˚C - 338˚C and the first wei ght loss is 0.2 5 mg in citric acid used LSCM in range 30˚C - 334˚C. The second weight loss is 0. 9 mg in NT P used LS CM in the t emper- ature range 490˚C - 822˚C, whereas the second weight loss is 0.42 mg in citric ac id used LSCM in range 334˚C - 688˚C. The second weight loss was attributed to the reac- tion between the residual nitrate and carriers after the decomposition of the precursor and subsequent combus- tion of organic components. The morphologies of La0.75 Sr0.2 5 Cr0.5Mn0. 5O3 -δ pe- rovskite nan-oparticles synthesized using different car- 02004006008001000 1200 1400 3.5 4.0 4.5 5.0 5.5 6.0 0.42mg 0.25mg 0.2mg 0.9mg LaSrCrMnO 3 +NTP LaSrCrMnO 3 + C it iric Ac id LaSrCrMnO 3 + Ox a lic Acid W eight loss/mg Temperature/ O C 0.32mg Figure 3. TGA curves of La0.75 Sr0.25Cr0. 5Mn0.5O3-δ (LSCM) perovskite gel precursor dried at 120ºC and then fired at 350˚C for 1h. (a) (b) (c) Figure 4. SEM images of La0.75Sr0.25Cr0.5Mn0.5O3-δ perovs- kite phase nanoparticles (a) NTP-assisted, (b) oxalic acid assisted and (c) citric acid assisted. 1μm 1μm 1μm ![]() Synthesis and Characterization of La0.75Sr0.25Cr0.5Mn0.5O3-δ Nanoparticles Using a combustion M ethod for Solid Oxide Fuel Cells Copyright © 2011 SciRes. NJGC 61 riers by combustion method as examined with scanning electron microscopy are show n in Fig ure 4. NTP-assisted LSCM shows many nanosized particles of sphe ricalshape in the range 100 - 500 nm (Figure 4(a)). The LSCM powders synthesized using oxalic acid and citric acid as carriers consist of uniform nanoparticles shwoing less agglomeration. The average particle size of the La0.75Sr0. 25Cr0.5Mn0.5O3-δ perovskite powders calcinated at 1200˚C is about 50 - 500 nm (Figures 4(a) and (b)). The small size La0.75Sr0.25Cr0.5Mn0.5O3-δ perovskite nano- particles are very active, small size is also beneficial for decreasing the fabrication temperature of the anode film and enhancing the catalytic proper ties. 4. Conclusions La0.75Sr0. 25Cr0.5Mn0.5O3-δ (LSCM) perovskite phase na- noparticles were successfully synthesized by solution combustion method using different carriers (NTP, oxalic acid, and citric acid) after calcination of fired gel at 1200˚C for 7 h. Scanning electron microscopy of the as-synthesized powders showed spherical particle shapes and sizes in the range of 50 - 500 nm. An exothermic reaction between carriers and nitrates initiates the com- bustion process. TGA and DSC analysis confirmed the decomposition process of nitrates and the organic matter. The combustion reactions took place in the temperature range 200 ˚C to 400˚C. 5. Acknowledgements One of the authors (V S Reddy Channu) thanks the Al- exander von Humboldt Foundation for a fellowship. 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