Parametric optimization and prediction of enhanced thermoelectric performance in co-doped CaMnO3 using response surface methodology and neural network
In this work, two different combinations of materials are prepared, and the effects on dual doping in Ca 1− x − y Gd x Sr x MnO 3 and Ca 1− x − y Ce x Sr x MnO 3 ( x = 0, 0.025, 0.05, y = 0, 0.025, 0.05) materials are evaluated, and its parameters are optimized and predicted by the Box-Benhken des...
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Veröffentlicht in: | Journal of materials science. Materials in electronics 2023-07, Vol.34 (21), p.1589, Article 1589 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | In this work, two different combinations of materials are prepared, and the effects on dual doping in Ca
1−
x
−
y
Gd
x
Sr
x
MnO
3
and Ca
1−
x
−
y
Ce
x
Sr
x
MnO
3
(
x
= 0, 0.025, 0.05,
y
= 0, 0.025, 0.05) materials are evaluated, and its parameters are optimized and predicted by the Box-Benhken design in the RSM method. The activation energy was measured with respect to different thermoelectrical material concentrations. RSM design is validated using hybrid DBN-RSO. The results show that increasing temperature, increases the amount of doping, decreases the thermal conductivity (k) and increases the electrical conductivity (σ) and power factor (PF). A bigger number of merits was also reached by increasing the amount of doping and the temperature. At 1000 K, the Ca
0.95
Gd
0.05
Sr
0.05
MnO
3
material has a low thermal conductivity and the highest figure of merit (ZT) value of 0.24, which is more than Ca
0.95
Ce
0.05
Sr
0.05
MnO
3
. The predicted values from the DBN-RSO method provide results that are closer to the experimental observations. The highest score (ZT) that the DBN-RSO prediction received was 0.26. Besides, the regression value of 99% is obtained from the experimented and predicted values. It shows the confidence and fitness of values. Also, the DBN-RSO achieves closer results to the experimental design with the lowest error value. |
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ISSN: | 0957-4522 1573-482X |
DOI: | 10.1007/s10854-023-10954-1 |