Cargando…
Performance of Segmented Thermoelectric Cooler Micro-Elements with Different Geometric Shapes and Temperature-Dependent Properties
In this work, the influences of the Thomson effect and the geometry of the p-type segmented leg on the performance of a segmented thermoelectric microcooler (STEMC) were examined. The effects of geometry and the material configuration of the p-type segmented leg on the cooling power ([Formula: see t...
Autores principales: | , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2018
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7512612/ https://www.ncbi.nlm.nih.gov/pubmed/33265209 http://dx.doi.org/10.3390/e20020118 |
Sumario: | In this work, the influences of the Thomson effect and the geometry of the p-type segmented leg on the performance of a segmented thermoelectric microcooler (STEMC) were examined. The effects of geometry and the material configuration of the p-type segmented leg on the cooling power ([Formula: see text]) and coefficient of performance ([Formula: see text]) were investigated. The influence of the cross-sectional area ratio of the two joined segments on the device performance was also evaluated. We analyzed a one-dimensional p-type segmented leg model composed of two different semiconductor materials, [Formula: see text] and [Formula: see text]. Considering the three most common p-type leg geometries, we studied both single-material systems (using the same material for both segments) and segmented systems (using different materials for each segment). The [Formula: see text] , [Formula: see text] and temperature profile were evaluated for each of the modeled geometric configurations under a fixed temperature gradient of [Formula: see text] T = 30 K. The performances of the STEMC were evaluated using two models, namely the constant-properties material (CPM) and temperature-dependent properties material (TDPM) models, considering the thermal conductivity ([Formula: see text]), electrical conductivity ([Formula: see text]) and Seebeck coefficient ([Formula: see text]). We considered the influence of the Thomson effect on [Formula: see text] and [Formula: see text] using the TDPM model. The results revealed the optimal material configurations for use in each segment of the p-type leg. According to the proposed geometric models, the optimal leg geometry and electrical current for maximum performance were determined. After consideration of the Thomson effect, the STEMC system was found to deliver a maximum cooling power that was [Formula: see text] higher than that of the single-material system. The results showed that the inverse system (where the material with a higher Seebeck coefficient is used for the first segment) delivered a higher performance than the direct system, with improvements in the [Formula: see text] and [Formula: see text] of [Formula: see text] and [Formula: see text] , respectively. Finally, analysis of the relationship between the areas of the STEMC segments demonstrated that increasing the cross-sectional area in the second segment led to improvements in the [Formula: see text] and [Formula: see text] of [Formula: see text] and [Formula: see text] , respectively. |
---|