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بناء وتوصيف BNT - BKT - BT البيزوالكترك لخزن الطاقة == Construction and Characterization of BNT - BKT - BT Piezoelectrics for Energy Harvesting
Author name:
نذير بشير محمود
Supervisor name:
عماد خضير الشكرجي
General topic:
Physics
Specific topic:
Physics
Degree:
Master
University:
Al-Nahrain University - College Of Science - Physics Department
Language:
English
University location:
Baghdad
First pages:
26T1737 - p.pdf
Abstract:
Lead - free piezoelectrics are non - toxic, cheap and environmental friendlymaterials. Among them Bismuth Sodium Titanate (BNT) which has thechemical formula Bi0.5Na0.5TiO3 with a complex A - site perovskite structure. Inthis study, some modifications on BNT were used to help in applications byforming solid solution with Bi0.5K0.5TiO3 (BKT) and BaTiO3 (BT). The BNTbased(xBNT - yBKT - zBT) with x+y+z=1 ; were prepared via different methodsat the Morphotropic Phase Boundary (MPB) : 0.94BNT - 0.06BT , 0.93BNT - 0.07BT , 0.8BNT - 0.2BKT, 0.84BNT - 0.16BKT and 0.9BNT - 0.065BKT - 0.035BKT with their origin BNT , BKT and BT. Mini Database was proposeddepending on the results of international databases and some crystallographysoftware and plotted as phase diagrams. Several predictions were suggesteddepending on the built Mini Database and phase diagrams for the BNT - BKTBTsystem. The main prediction was : the physical properties either dependedon the changing of crystal structure ( polarization , dielectric constant ,piezoelectric coefficient ) or the properties had linearity with the composition (density, melting point , sintering temperature ). It has been focused on thestudying the crystal structure, dielectric measurements, hysteresis loopmeasurements and polarization fatigue analyses for ceramic samples.The samples were prepared by different methods : the hydrothermalmethod with spherical shape particles of 65nm - 600nm size; and by solid statereaction method. The powder were pressed in suitable template at 250MPa ,sintered according to database prediction "sintering temperature phase diagram", the resulted ceramic discs had relative density 90% - 96 %. These results agreed with the database predictions "sintering and density phase diagrams”.The crystal structure for the prepared samples were studied using X - ray diffraction (XRD) analysis, the XRD showed that the samples BNT - 6BT, BNT - 7BT, BNT - 20BKT, BNT - 16BKT and BNT - BKT - 35BT had the Morphtropic Phase Boundary (MPB) while BNT had the rhombohedral structure. BKT and BT had a tetragonal structure. These results agreed with the predictions "crystal structure phase diagram" The dielectric measurements showed that there were three regions for BNT - BKT - BT system; the first one was the samples with relaxor ferroelectric behaviors, the samples belonging to this region were BNT, BNT - 6BT, BNT - 7BT, BNT - 20BKT, BNT - 16BKT and BNT - BKT - 35BT (i.e. BNT and the MPB region). The second region was the samples with Normal ferroelectric behavior.The sample with this region was BT. The third region was the samples with relaxor - like ferroelectric behavior (weak ferroelectric) as in BKT. The Curie temperature for the samples within MPB was between 270℃ to 300℃, while for the origin : for BNT the Curie temperature was about 320℃; for BKT was about 370℃; and for BT was about 110℃. The depolarization temperature for samples within MPB region was below 100℃ (above room temperature) while for BNT was 250℃.The hysteresis loop measurements were studied both experimentally and theoretically. The study showed that the results for BNT were Ps=35μC/cm2, Ec=60kV/cm, for BKT was Ps=30μC/cm2, Ec=4.7kV/cm and for BT was Ps=26μC/cm2, Ec=9.8kV/cm, while for the samples within the MPB region the results were Ps=45μC/cm2, Ec ≈ 30kV/cm. The polarization had the largest value within MPB, which agreed with the first prediction by the proposed database (i.e. the polarization of BNT - BKT - BT system depends on crystal structure). The coercive electric (Ec) had a linear behavior with the composition. The value of Ec within MPB was in the range of 27kV/cm to 33kV/cm, which was half of the value for pure BNT. This result agreed with the second prediction by thedesigned database. The polarization fatigue analyses were performed depending on the fatigue model. The results showed that the polarization life cycle had the values of 1012 cycles for BNT, 1011 cycles for BT and 104 cycles for BKT, while within MPB region the polarization life had the largest value of about 1016 cycles which was much greater than in origin (BNT, BKT and BT). This result also agreed with the first prediction by the designed database (polarization life cycle had the largest value and depends on the crystal structure). The fatigue analyses predicted the value of applied electric field used in hysteresis loop measurements and the effect of cycle on the applied electric field.Finally, some of the problems were skipped and properties of BNT were enhanced by looking for the MPB region in the solid solution. The MPB showed the value for polarization to be larger than that in pure BNT, and it reduced the coercive electric field comparing to the original BNT. The polarization life cycle at MPB was much greater than in BNT. Therefore, this study could find some solutions for the drawbacks of BNT, and solve some problems for other piezoelectrics.
