| People | Locations | Statistics |
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| Naji, M. |
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| Motta, Antonella |
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| Aletan, Dirar |
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| Mohamed, Tarek |
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| Ertürk, Emre |
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| Taccardi, Nicola |
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| Kononenko, Denys |
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| Petrov, R. H. | Madrid |
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| Alshaaer, Mazen | Brussels |
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| Bih, L. |
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| Casati, R. |
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| Muller, Hermance |
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| Kočí, Jan | Prague |
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| Šuljagić, Marija |
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| Kalteremidou, Kalliopi-Artemi | Brussels |
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| Azam, Siraj |
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| Ospanova, Alyiya |
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| Blanpain, Bart |
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| Ali, M. A. |
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| Popa, V. |
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| Rančić, M. |
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| Ollier, Nadège |
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| Azevedo, Nuno Monteiro |
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| Landes, Michael |
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| Rignanese, Gian-Marco |
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Rosendahl, Lasse
Aalborg University
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (18/18 displayed)
- 2022Online Condition Monitoring of Rotating Machines by Self-Powered Piezoelectric Transducer from Real-Time Experimental Investigationscitations
- 2021The investigation of viscous and structural damping for piezoelectric energy harvesters using only time-domain voltage measurementscitations
- 2021Continuous co-processing of HTL bio-oil with renewable feed for drop-in biofuels production for sustainable refinery processescitations
- 2020Design Optimization of Waste Heat Recovery System around Cement Rotary Kilncitations
- 2020Catalytic Hydrothermal Liquefaction of Eucalyptus: Effect of Reaction Conditions on Bio-oils Properties.
- 2020A comprehensive electromechanically coupled model for non-uniform piezoelectric energy harvesting composite laminatescitations
- 2020A broadband macro-fiber-composite piezoelectric energy harvester for higher energy conversion from practical wideband vibrationscitations
- 2019On the effect of driving amplitude, frequency and frequency-amplitude interaction on piezoelectric generated power for MFC unimorph
- 2019An Experimental Study on Macro Piezoceramic Fiber Composites for Energy Harvestingcitations
- 2017Two-stage alkaline hydrothermal liquefaction of wood to biocrude in a continuous bench-scale systemcitations
- 2017Experimental Investigation of Zinc Antimonide Thin Film Thermoelectric Element over Wide Range of Operating Conditionscitations
- 2016Flash calcination of kaolinite rich clay and impact of process conditions on the quality of the calcines:A way to reduce CO2 footprint from cement industrycitations
- 2016Experimental Investigation of Zinc Antimonide Thin Films under Different Thermal Boundary Conditions
- 2016Power Generation by Zinc Antimonide Thin Film under Various Load Resistances at its Critical Operating Temperature
- 2016Flash calcination of kaolinite rich clay and impact of process conditions on the quality of the calcinescitations
- 2015Experimental and modeling study of flash calcination of kaolinite rich clay particles in a gas suspension calcinercitations
- 2014Simulation of flash dehydroxylation of clay particle using gPROMS:A move towards green concretecitations
- 2014Simulation of flash dehydroxylation of clay particle using gPROMScitations
Places of action
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article
Experimental Investigation of Zinc Antimonide Thin Film Thermoelectric Element over Wide Range of Operating Conditions
Abstract
Zinc antimonide compounds are among the most efficient thermoelectric (TE) materials with exceptional low thermal conductivity at moderate temperatures up to 350 °C. This study aims to evaluate the performance of a zinc antimonide thin film TE deposited on an insulating substrate, while the heat flows in plane with the thin film. At first, the effect of applying different temperatures at the hot side of the specimen is investigated to reach steady state in an open circuit analysis. Then, the study focuses on performance and stability analysis of the thermoelectric element operating under different resistive loads and over a wide range of operating temperatures from 160 °C to 350 °C. The results show that, at a hot side temperature equal to 275 °C, the Seebeck coefficient (α) reaches its maximum value (242 μV/K), which is comparable to that of bulk materials reported in the literature. According to a variation of the load resistance, the maximum power output, that is a function of temperature, occurs at 170.25 Ω. The maximum power is 8.46 μW corresponding to a cold and hot side temperature of ≈ 30 °C and 350 °C, respectively.