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<p class="art-type" id="articleinfo">Research Article</p>
<p class="art-title">Preparation and Characterization of Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub> Cathode for Solid Oxide Fuel Cell</p>
<p class="art-author">Rajasekhar M<sup>*</sup>, and Kalaivani N</p>
<p class="art-affl">Advanced Energy Research Lab, PG & Research Department of Chemistry, Government Arts College, Dharmapuri, India</p>
<p class="art-aff"><b>*Corresponding author: Mari Rajasekhar</b>, Advanced Energy Research Lab, PG & Research Department of Chemistry, Government Arts College, Dharmapuri, India, E-mail: <a href="mailto:drmrchem@gmail.com">drmrchem@gmail.com</a></p>
<p class="art-aff"><b>Received</b>: July 23, 2018 <b>Accepted</b>: September 20, 2018 <b>Published</b>: September 26, 2018</p>
<p class="art-aff"><b>Citation</b>: Rajasekhar M, Kalaivani N. Preparation and Characterization of Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub> cathode for Solid Oxide Fuel Cell. <i>Madridge J Nanotechnol Nanosci</i>. 2018; 3(2): 112-115. doi: <a href="https://doi.org/10.18689/mjnn-1000121">10.18689/mjnn-1000121</a></p>
<p class="art-aff"><b>Copyright</b>: &copy; 2018 The Author(s). This work is licensed under a Creative Commons Attribution 4.0 International License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.</p>
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					<p class="art-subhead" id="abstarct">Abstract</p>
					<p class="art-para">Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub> (0 &#8804; x &#8804; 0.5) cathode materials are synthesized with Gd(NO<sub>3</sub>)<sub>3</sub>, Sr(NO<sub>3</sub>)<sub>2</sub>,Al(NO<sub>3</sub>)<sub>3</sub>, and aspartic acid (fuel) by assisted combustion method with heating at 550&#176;C for 6 hours. The surface morphology of the synthesized crystalline powder is characterized by Scanning Electron Microscopy (SEM). Thus, particle size and porosity were determined. The synthesis and crystallization are followed by thermochemical techniques (TGA/DTA) studies. The synthesized materials showed reasonable electrical conductivity. These results indicate that assisted combustion method is a promising method to prepare nanocrystalline Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub> for solid oxide fuel cell.</p>
<p class="art-para"><b>Keywords:</b> Ionic conductivity; Scanning Electron Microscopy; Transmission Electron Microscope; Thermal Analysis.</p>
<p class="art-subhead" id="intro">Introduction</p>
<p class="art-para">Fuel cells are electrochemical device that converts the chemical energy of a directly into electricalenergy. The challenge is to develop material with good performance at intermediate temperature (500-800&#176;C) for SOFCs allowing to reduce the cost of the cell and increasing the long-term stability.For the fuel cell, the most commonly used materials are lanthanum strontium manganite (LSM) was used for the cathode, YSZ for the electrolyte and Ni&#8211;YSZ cermet for the anode. It is essential that the chosen interconnect material have highest chemical stability, the highest oxidation resistance as well as the highest electrical conductivity.</p>
<p class="art-para">The permanent increment of human population is accompanied by increase of energy demand and more restrictive environmental regulations. In that instance, the Solid Oxide Fuel Cells (SOFC) technology has emerged as an efficient substitution of the presently existing energy devices. Fuel cells are important type of electrochemical devices which converts chemical energy into electrical energy in aclean and calm way. Assisted combustion synthesis (ACS) or self-propagating high-temperature synthesis (SHS) is an effective, low-cost method for production of various industrially useful materials. They have wide range of potential applications ranging from providing power for portable devices (eg. Mobile phones, laptop computers) and transport applications to small and large scale stationary power applications.</p>
<p class="art-para">The assisted combustion method is a novel method in the production of ultra-fine ceramic powders with a small particle size and high porosity <a href="#1" id="ref1">[1</a>-<a href="#2" id="ref2">2]</a>. Fuel cells have many advantages compared to conventional electric power generation systems such as high conversion efficiency which is relatively independent of size as well as environmental compatibility.</p>
<p class="art-subhead">Experimental Studies</p>
<p class="art-para">The nanocrystalline Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub> powder was synthesized by assisted combustion method using high purity of Gd(NO<sub>3</sub>)<sub>3</sub>, Sr(NO<sub>3</sub>)<sub>2</sub>, Al(NO<sub>3</sub>)<sub>3</sub> and aspartic acid as fuel. All the reagents were purchased from Sigma Aldrich, &gt;99.9%), the required stoichiometric amounts of the starting materials were dissolved in double distilled deionized water in order to obtain a homogeneous solution. This solution was kept at constant heating at 80&#176;C to obtain the foamy powders of Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub> is show in AS <a href="#f001">Figure 1</a>. For Calcination, the foamy powder was carried out in a muffle furnace at 550&#176;C for six hours <a href="#3" id="ref3">[3</a>-<a href="#4" id="ref4">4]</a>.</p>
<div class="art-img" id="f001">
<img src="<?php echo $imgpath;?>images/mjnn-121-f001.gif" class="img-responsive center-block"/></div>
<div class="text-center"><b>Figure 1</b>. Flow chart of assisted combustion synthesis of Gd<sub>1-x</sub>Sr<sub>x</sub>AlO<sub>3</sub></div>
<p class="art-subhead">Characterization analysis</p>
<p class="art-para">X-ray powder diffraction (XRD) data were collected at room temperature with a diffractometer (Model: Philips X&#700; Pert MPH<sup>R</sup>) with Cu K&#945; radiation. The data were recorded in the 2&#952; range of 10-70 with a 0.02&#176; steps. The particle size and morphology of the produced powderwas analysed with a JEOL scanning electron microscopy SEM (Model: JSM-840A) equipment with INCA was used to determine the morphology of samples.</p>
<p class="art-para">The thermal decomposition of the polymeric precursors was characterized by Perkin-Elmer TG/DTA thermal analysis (Model; Pyris Diamond). The TGA is a process which relies on measuring the change in physical and chemical properties of a sample as a function of temperature (with constant heating rate) or as a function of time (with constant temperature). It is predominantly used for determining the features of a material that exhibit either mass loss or gain due to decomposition, oxidation or loss of volatiles. Differential thermal analysis is a technique in which the temperature of a sample is compared with an inert reference material during the programmed change of temperature <a href="#5" id="ref5">[5]</a>.</p>
<p class="art-para">The particle size of the synthesized powder was observed by means of a JOEL transmission electron microscopy (Model: 1200 EX). The synthesized powder was analysed with FTIR spectrometry. (Agilent Cary 630 FTIR spectrometer) and which scanned in a region of about 4000-400cm<sup>-1</sup>. The ionic conductivity of the sintered pellets were measured by a dc-four probe method in which temperatures range 200-700&#176;C in air.</p>
<p class="art-subhead" id="discussion">Results and Discussion</p>
<p class="art-para"><b>Analysis of Crystalline Structure</b></p>
<p class="art-para">The powder XRD analysis was performed on the prepared Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub> nanocrystalline powders at 550&#176;C for 6 hours. It was used for identifying the crystallite size of Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub> powder. The perovskite phase has existed in the resulting powder but the impurity phase has exist clearly as well. In general, all the diffracted peaks are broader than usually observed for highly crystalline powder. The broadening in the diffracted peaks is attributed to the superfine crystalline nature of composites. The size of the particles were calculated by Scherrer equation, it was 30 nm <a href="#6" id="ref6">[6</a>-<a href="#8" id="ref8">8]</a> as shown in <a href="#f002">Figure 2</a>.</p>
<div class="art-img" id="f002">
<img src="<?php echo $imgpath;?>images/mjnn-121-f002.gif" class="img-responsive center-block"/></div>
<div class="text-center"><b>Figure 2</b>. X-ray diffraction pattern of Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub></div>
<p class="art-para"><b>SEM analysis:</b></p>
<p class="art-para"><a href="#f003">Figure 3</a>. shows the SEM microstructure of Gd<sub>0.7</sub>Sr<sub>0.3</sub>AlO<sub>3</sub> powder obtained at 550&#176;C for 6 hours. The surface morphology of the synthesized product is different pores and grains. Further, the SEM image indicates that the particles are agglomeration. All the samples are relatively dense and do not show much difference in density. However Sr doping significantly improves the grain growth. The average grain size of the doped samples is between 4 and 12 &#956;m. The average crystallite size is 30 nm. The particles are uniformly distributed. There is agglomeration of the particles. The particles of the synthesized products are in nanorange <a href="#9" id="ref9">[9]</a>.</p>
<div class="art-img" id="f003">
<img src="<?php echo $imgpath;?>images/mjnn-121-f003.gif" class="img-responsive center-block"/></div>
<div class="text-center"><b>Figure 3</b>. TGA & DTA of Gd<sub>0.7</sub>Sr<sub>0.3</sub>AlO<sub>3</sub></p>
<p class="art-para"><b>Thermal Analysis of TGA/DTA</b></p>
<p class="art-para"><b><a href="#f004">Figure 4</a></b>. shows that the TGA/DTA pattern obtained on Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub> powder. The sample heating from 100&#176;C-800&#176;C which shows slight weight loss of about 0.035mg/min. Again the sample shows a weight increase from 105.3&#176;C -386.39&#176;C of 0.070mg/min. The weight gain and weight loss indicated that the Gd0.7Sr0.3AlO3 powder exhibited easy reversible absorbtiondesorbtion of oxygen from air. The weight loss is minimum because of the removal of residual H<sub>2</sub>O and different gases. The chemical decomposition with an increases of temperature was examined through DTA and it appeared as the endothermic and exothermic peaks. From the above TGA/DTA data, know the Gd<sub>0.7</sub>Sr<sub>0.3</sub>AlO<sub>3</sub> gradually absorbs the oxygen from air with temperature <a href="#10" id="ref10">[10]</a>.</p>
<div class="art-img" id="f004">
<img src="<?php echo $imgpath;?>images/mjnn-121-f004.gif" class="img-responsive center-block"/></div>
<div class="text-center"><b>Figure 4</b>. TGA & DTA of Gd<sub>0.7</sub>Sr<sub>0.3</sub>AlO<sub>3</sub></div>
<p class="art-para"><b>FTIR Analysis</b></p>
<p class="art-para">FTIR spectroscopy was used to confirm metal oxide bond formation in the crystal and is investigated their vibrational behavior in solid state of Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub> powder. It was recorded in the range of 4000 cm<sup>-1</sup> to400 cm<sup>-1</sup>. The infrared spectrums of synthesized samples of Gd<sub>0.7</sub>Sr<sub>0.3</sub>AlO<sub>3</sub> powder are shown in <a href="#f005">Figure 5</a>. The broad band at 1437.7cm<sup>-1</sup> is assigned to vibration mode of chemically bonded hydroxyl groups. The peak appeared at 853.0 cm<sup>-1</sup> corresponds to the H-O-H bond mode confirming the presence of moisture in the sample. The peak appeared at 1437.7 cm<sup>-1</sup> is due to the presence of CO<sub>2</sub> in the sample. The Gd<sub>0.7</sub>Sr<sub>0.3</sub>AlO<sub>3</sub> exhibited a low intensity peak at 704.8 cm<sup>-1</sup> and the sample exhibited three peaks obtained between the wavelength regions 600-1000 cm<sup>-1</sup> which observed at 853.0, 723.8, and 704.8cm<sup>-1</sup>. The peak appeared at 1437.7 cm<sup>-1</sup> is related to the O-H stretching vibration of H<sub>2</sub>O in the sample. The broad band at 1437.7 cm<sup>-1</sup> is assigned to vibration mode of chemically bonded hydroxyl groups.</p>
<div class="art-img" id="f005">
<img src="<?php echo $imgpath;?>images/mjnn-121-f005.gif" class="img-responsive center-block"/></div>
<div class="text-center"><b>Figure 5</b>. FT-IR spectrum of Gd<sub>0.7</sub>Sr<sub>0.3</sub>AlO<sub>3</sub></div>
<p class="art-para"><b>Conductivity</b></p>
<p class="art-para"><a href="#f006">Figure 6</a>. shows that the Arrhenius plots of conductivity for Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub> samples sintered at different temperature range. It can be seen from <a href="#f006">Figure 6</a>, that the conductivity of the samples increases gradually with increasing the temperature. In this case, grains grow excessively, and the pores are trapped among the grains or grain boundaries, blocking oxygen ion migration leading to the decreases in the conductivity of the sample. The volatilization of gaseous SrO and O<sub>2</sub> from Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub> at excessively high sintering temperature were detected by mass spectroscopy resulting in the sample volumes bloating and density reduction, so that the conductivity decreases.</p>
<div class="art-img" id="f006">
<img src="<?php echo $imgpath;?>images/mjnn-121-f006.gif" class="img-responsive center-block"/></div>
<div class="text-center"><b>Figure 6</b>. Arrhenius plots for the Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub> samples sintered at different ratios</p>
<p class="art-subhead">Conclusion</p>
<p class="art-para">The present investigation was carried out to improve the performance of Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub> by the synthesis method. The electrochemical behavior of Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub>based on the method of synthesis and sintering temperature. The present work was mainly focused on synthesis, and ionic conductivity of Gd<sub>1-x</sub>S<sub>rx</sub>AlO<sub>3</sub>.</p>
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