4.7 Article

Simulation of heat loss in Cu2ZnSn4SxSe4_x thin film solar cells: A coupled optical-electrical-thermal modeling

期刊

RENEWABLE ENERGY
卷 181, 期 -, 页码 320-328

出版社

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.renene.2021.09.035

关键词

Cu2ZnSn4SxSe4-x; Heat generation; Thin film; Solar cells

资金

  1. Russian Government
  2. Research Institute of Mechanical Engineering. Department of Vibration Testing and Equipment Condition Monitoring, South Ural State University, Chelyabinsk, Russian Federation

向作者/读者索取更多资源

A coupled optical-electrical-thermal modeling was developed to investigate heat generation and dissipation in Cu2ZnSn4SxSe4-x thin film solar cells. The study found that thermalization is the dominant heat generation factor, while factors like Joule heat, non-radiative recombination heat, and surface recombination heat also play important roles. Temperature increases during operation, affecting the fill factor and power conversion efficiency.
A coupled optical-electrical-thermal modeling has been developed to investigate the heat generation and dissipation in Cu2ZnSn4SxSe4-x thin film solar cells. Five heat generation factors: Thermalization, Joule heat, Peltier heat, Surface Recombination heat, and non-radiative recombination heat (Shockley-Read Hall and Auger) as well as two heat dissipation factors convective and radiative cooling were calculated and displayed in 2 and 3 dimensional maps. Thermalization is the dominant heat generation factor in the cell independent of the voltage. The non-radiative recombination heat and Joule heat depend on voltage. Apart from these bulk heating factors, the surface recombination heat and Peltier heat were also investigated. The surface recombination heat is higher at open-circuited voltage (V=V-oc) compared to at V = 0 while the Peltier heat is zero at V=V-oc which can be explained by looking at the energy band diagrams at these voltages. The total heat generation has a small gradient across the cell thickness (<5 x 10(9) W/m(3)) as the cell is quite thin. However the Voc decreases from 0.54 V to 0.49 V (DV = 0.047 V). The temperature shows small gradient across the cell (0.01 K). However, the initial temperature (293 K) increases to 315-320 K during the operation as studied by the coupled study. A higher temperature did not change the Jsc but the fill factor decreases from 73.8% to 71.8% and the PCE falls by 11.11% (from initial 12.78%-11.36%). All the total heat dissipation, convective, and radiation cooling follow a similar trend to the total heat generation but convective cooling is the dominant component of dissipation. We compared our simulation results with literature data for heat impact on device characteristics of kesterite thin film solar cells. (C) 2021 Elsevier Ltd. All rights reserved.

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