Elsevier

Nano Energy

Volume 76, October 2020, 105117
Nano Energy

Predicting performance of fiber thermoelectric generator arrays in wearable electronic applications

https://doi.org/10.1016/j.nanoen.2020.105117Get rights and content

Highlights

  • Models of three-dimensional array generator with a low temperature difference under conductive and radiative heat transfer.

  • Quantified influences of materials, device structure and application conditions on output performance of the device.

  • Theoretical upper limits of performance of the device worn on human back at various ambient temperatures.

Abstract

Emerging fiber-based thermoelectric generators have shown great potentials to power wearable electronics by harvesting thermal energy from human body and environment. However, the lack of quantitative analytical tools has hindered the research progress, particularly related to their design and evaluation, covering selection and optimization of thermoelectric, electric and structural materials, device structure, fabrication processes and application conditions. Here, we report a quantitative approach to predict the performance of three-dimensional fiber-based thermoelectric generators composed of one-dimensional fiber generator array, working under conductive and radiative heat transfer conditions with a low temperature difference. We first present an experimentally verified model of single fiber generator unit, consisting of core/sheath fiber leg and electrodes, to quantify the effects of the material properties and structural parameters on the output power and energy conversion efficiency of the fiber unit. Then we propose a second model of three-dimensional fiber-based thermoelectric array generator to predict its output performance in terms of fiber unit packing density and surface emissivity. Finally, the theoretical upper limits of output power and conversion efficiency are given for the fiber-based thermoelectric array generators worn on a human torso back under a range of ambient temperature.

Introduction

Fiber-based thermoelectric generators (FTEGs) are flexible, conformable and light-weight devices, which can directly convert heat into electricity without any moving parts or working fluids [1]. At present, the output performance of such devices is generally lower, in the range of ~1 μW/cm2, close to body temperature with a small temperature difference, say ~15 K [2,3]. These devices are great candidates to provide energy to the wearable electronics. To this end, high output power and energy conversion efficient are essential for FTEGs in wearable applications. However, up to date, there is no quantitative analytical tool that can guide the engineering design of FTEGs, including selection of thermoelectric (TE), electric and structural materials, the device structure and fabrication processes with particular application conditions.

To achieve high energy conversion efficiency of rigid thermoelectric generators (TEGs), significant progress has been made to explore TE materials of high figure of merit, ZT=σα2T/κ, where σ is the electrical conductivity; α is the Seebeck coefficient; T is the temperature; κ is the thermal conductivity [[4], [5], [6], [7], [8], [9]]. For the power generation application, these materials include Bi2Te3 and its alloy [10], silicides [11], PbTe [[12], [13], [14]], half-Heusler [15], poly(3,4-ethylenedioxythiophene): poly(styrenesulfonate) (PEDOT: PSS) [16], and graphene and composites [17]. The theoretical studies of traditional TEGs have been conducted for solid cuboid structure, usually with a large temperature difference and under conditions of conductive heat transfer [[18], [19], [20]]. These models have provided important engineering design guidelines in traditional rigid TEGs by changing the cross-sectional area, length and segment of solid p- and n-type TE legs for the high output performance [[21], [22], [23], [24]]. However, these models cannot be applied in the wearable applications where the temperature at one end is fixed but at the other end is free. For example, the surface temperature of human torso can be regarded as a constant. Under this condition, the temperature at the other end is the result of the heat transfer.

Three-dimensional (3D) spacer fabric structure may offer high specific output power from the FTEGs because of the light weight and the large temperature difference between the face and back sides connected by numerous one-dimensional (1D) FTEG units1. The output performance of the 3D FTEGs is determined by those of 1D FTEGs. Compared with the thick TE columns in traditional rigid TEG arrays, the 1D FTEG units have much higher aspect ratio, which results in the large deformability and flexibility. A recent work reported 3D space fabric FTEGs comprising 1D FTEG units where the core was a carbon nanotube yarn (CNTY) acting as a continuous electrode3. The sheath was coated with p-type PEDOT: PSS and n-type polyethyleneimine (PEI). It is not desirable that in the FTEGs much thermal energy was conducted from the hot to cold end through the CNTY of high thermal conductivity. Therefore, higher performance of the FTEG can be achieved with a more appropriate consideration of materials and device structure, ideally guided by a quantitative analytical tool.

Hence, this paper presents a quantitative approach to predict the performance of 3D FTEG composed of 1D FTEG array in simulated wearable conditions, that is, under conductive and radiative heat transfer with low temperature differences. The single 1D FTEG unit, consisting of core/sheath fiber TEG leg and electrodes, is dealt with under conduction and radiation heat transfer. The influences of the radius and the length of filament, the thickness of TE coating layer, the distance between the adjacent surfaces of 1D FTEGs and the surface emissivity are quantified. Finally, the upper limits of output power and conversion efficiency of the FTEG array device with various TE materials are given if worn on a human torso back under a range of ambient temperature.

Section snippets

Mathematical model

FTEG devices convert thermal energy into electrical energy according to the Seebeck effect. Fig. 1(a) illustrates a 1D FTEG unit comprising a polymer core filament coated with TE material in the middle and conductive material at its both ends. Based on the Seebeck effect, the equivalent voltage source, U, induced by the temperature difference can be estimated by the following equationU=αΔTwhere α is the Seebeck coefficient of TE material, ΔT is the temperature difference between the hot and

Influencing factors on performance of 1D FTEG array

In this section, for quantifying the importance of factors, the single 1D FTEG is studied under conductive and radiative heat transfer at first. Then, the 1D FTEG array formed by the single ones is investigated with the consideration of the influence of the controlled parameter.

Upper limit of performance of array devices

Suppose the 3D FTEG composed of 1D FTEG arrays is worn on the back of a human with the surface temperature of around 35°C, as shown in Fig. 1(b). The ambient temperature is in the range of 55°C~55°C. The model in Section 3.2 is applied to investigate the upper limit of the performance of the 1D FTEG array composed of different TE materials (in Table 1) under different ambient temperature. The control parameter and the emissivity of the 1D FTEG array are 1 and 0.5, respectively. The

Conclusion

This paper reports new theoretical models for 1D FTEGs and 3D FTEG array device, working under conductive and radiative thermal transfer with a low temperature difference comparable to wearable applications, and their numerical simulation results. The influences on output power and energy conversion efficiency of the FTEGs have been given in terms of the fiber dimension, the thickness of TE coating layer, packing density of the array and the surface emissivity. The theoretical model for single

CRediT authorship contribution statement

Li-sha Zhang: Conceptualization, Formal analysis, Investigation, Validation, Visualization, Writing - original draft. Bao Yang: Conceptualization, Methodology. Shu-ping Lin: Investigation, Methodology. Tao Hua: Supervision. Xiaoming Tao: Conceptualization, Data curation, Funding acquisition, Methodology, Resources, Supervision, Writing review & editing.

Declaration of competing interest

The authors declare that there is no conflict of interests.

Acknowledgements

The work has been partially supported by Research Grants Council, Hong Kong, China (Grant No. 15201419E, 15200917E, 15204715E) and Hong Kong Polytechnic University (Grant No. AAB3 and 847A). L.Z. acknowledges a postgraduate scholarship from Hong Kong Polytechnic University.

References (42)

  • M. Takashiri et al.

    Fabrication and characterization of bismuth-telluride-based alloy thin film thermoelectric generators by flash evaporation method

    Sens. Actuators, A

    (2007)
  • W. Zhu et al.

    Hierarchical Bi-Te based flexible thin-film solar thermoelectric generator with light sensing feature

    Energy Convers. Manag.

    (2015)
  • L.M. Goncalves et al.

    Optimization of Bi2Te3 and Sb2Te3 thin films deposited by co-evaporation on polyimide for thermoelectric applications

    Vacuum

    (2008)
  • L.H. Fan et al.

    A comprehensive and time-efficient model for determination of thermoelectric generator length and cross-section area

    Energy Convers. Manag.

    (2016)
  • G. Zhang et al.

    A comprehensive design method for segmented thermoelectric generator

    Energy Convers. Manag.

    (2015)
  • Z.Q. Niu et al.

    Elucidating modeling aspects of thermoelectric generator

    Int. J. Heat Mass Tran.

    (2015)
  • B. Jang et al.

    Optimal design for micro-thermoelectric generators using finite element analysis

    Microelectron. Eng.

    (2011)
  • Z.L. Wang

    Toward self-powered sensor networks

    Nano Today

    (2010)
  • L. Zhang et al.

    Fiber‐based thermoelectric generators: materials, device structures, fabrication, characterization, and applications

    Adv. Energy Mater.

    (2018)
  • Y. Zheng et al.

    Carbon nanotube yarn based thermoelectric textiles for harvesting thermal energy and powering electronics

    J. Mater. Chem.

    (2020)
  • D. Byeon et al.

    Discovery of colossal Seebeck effect in metallic Cu2Se

    Nat. Commun.

    (2019)
  • Cited by (22)

    • High performance single material-based triboelectric nanogenerators made of hetero-triboelectric half-cell plant skins

      2022, Nano Energy
      Citation Excerpt :

      Such a difference in the intensity was found to be directly relevant to the output of TENGs, which will be discussed below. The triboelectric effects of organic and inorganic materials are usually characterized using different methods [4,32,33], and their charge affinities during the triboelectrification process could be estimated based on their physical properties, such as the work function [34] and the energy gap of the molecular orbitals [35]. However, biological materials cannot be easily estimated in that way because of the complexity of their chemical and biological structures.

    • WKYMVm ameliorates acute lung injury via neutrophil antimicrobial peptide derived STAT1/IRF1 pathway

      2020, Biochemical and Biophysical Research Communications
      Citation Excerpt :

      In fact, various ligands-based FPR2 conformational changes differentially exhibit proinflammatory response, including chemotaxis and the release of inflammatory cytokines or anti-inflammatory/pre-resolving response. Ye and colleagues reported that Ac2-26 the N-terminal of annexin AI for anti-inflammation and amyloid beta 42 for pro-inflammation are major modulators that are involved in the induction of distinct conformational changes of FPR2 through biased allosteric modulation [16]. Despite the modification of FPR2 by ligands, Fpr2-deficient mice developed susceptibility and bacteria load in the liver with reduced antimicrobial activity of the neutrophils against to Listeria monocytogenes [17].

    View all citing articles on Scopus
    View full text