Bringing Thermoelectricity Into Reality 2018
DOI: 10.5772/intechopen.75790
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Thermoelectric Devices: Influence of the Legs Geometry and Parasitic Contact Resistances on ZT

Abstract: In this chapter, the impact of the shape of thermoelectric legs and parasitic contact resistances from metal electrodes and device wiring on thermoelectric figure of merit ZT is addressed. First section deals with the influence of the legs geometry on ZT. The shape of the legs is crucial in the thermoelectric performance of the thermoelectric devices. Unlike to conventional geometry thermoelectric legs, non-constant cross-section legs could help by lowering the overall thermal conductance of the device so as t… Show more

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Cited by 6 publications
(5 citation statements)
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“…[99][100] Here, the Thomson effect, i. e. Thomson coefficient, t T ð Þ ¼ TdS dT ( Seebeck coefficient varies at different points along the length of the thermoelements) is harnessed which is otherwise neglected in the conventional cuboidal structure. [86] Thus, the output power demonstrates ~70% augmentation in the pyramidal structure in comparison to the cuboidal geometry, proving the significance of the geometrical layout of the thermoelectric legs in the device functioning.…”
Section: Flat Plate Cuboidal Thermoelectric Devicementioning
confidence: 90%
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“…[99][100] Here, the Thomson effect, i. e. Thomson coefficient, t T ð Þ ¼ TdS dT ( Seebeck coefficient varies at different points along the length of the thermoelements) is harnessed which is otherwise neglected in the conventional cuboidal structure. [86] Thus, the output power demonstrates ~70% augmentation in the pyramidal structure in comparison to the cuboidal geometry, proving the significance of the geometrical layout of the thermoelectric legs in the device functioning.…”
Section: Flat Plate Cuboidal Thermoelectric Devicementioning
confidence: 90%
“…[97] Recently, a pyramidal shaped prototype thermoelectric generator was assembled by Mijangaos et al and found that pyramidal legs i. e. asymmetrical thermoelements lower the thermal conductance, in turn, enhances the temperature gradient, alongside the legs as shown in Figure 7. [86] Moreover, Sahin and Yilbis also carried out detailed analysis of the impact of the geometry of the thermoelements on the efficiency and output power of thermoelectric power generators. [98] It has been analysed that thermoelectric performance of the trapezoid legs i. e. where the cross-section varies linearly gives more output power density than conventional rectangular leg geometry.…”
Section: Flat Plate Cuboidal Thermoelectric Devicementioning
confidence: 99%
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“…In practice, typical figures may be higher, between 10 −7 and 10 −5 • cm 2 [111]. As an example of the influence of electrical contact resistivity, the optimal film thickness of a TFTEC changes from 20 μm [83], [112] for contact resistivity in the order of 10 −6 •cm 2 to <2 μm when the contact resistivity decreases to 10 −8 •cm 2 [7]. For a 100× 100 μm 2 Si/SiGe TEC, an increase in contact resistivity from 10 −9 to 10 −4 •cm 2 degrades performance by ∼85%, whereas the same device scaled to a 3000 × 3000 μm 2 area would face only a ∼5% degradation [111].…”
Section: Influence Of Parasitic Effectsmentioning
confidence: 99%
“…al found that the power output of a TEG is maximized at a shorter leg length than that at which device efficiency is maximized [22]. Fabian-Mijanos and Alvarez-Quintana studied pyramidal-shaped semiconductor legs and found that maximum power output was almost two times greater than that of symmetric rectangular legs, which was accredited to the utilization of the Thomson effect [23]. While these works give insight on the effects of individual geometric parameters, the work presented herein eliminates the necessity for parametric studies by providing an algorithm that optimizes the semiconductor leg shape profile based on the realized temperature difference.…”
Section: Introductionmentioning
confidence: 99%