Nonlinear dynamics study of freestanding triboelectric nanogenerator system

被引:2
作者
Cao, Jingyu [1 ]
Bao, Jiusheng [1 ]
Yin, Yan [1 ,2 ]
Cao, Ting [1 ]
机构
[1] China Univ Min & Technol, Sch Mech & Elect Engn, Xuzhou 221116, Jiangsu, Peoples R China
[2] Chongqing Univ, State Key Lab Mech Transmiss Adv Equipment, Chongqing 400044, Peoples R China
关键词
triboelectric nanogenerator system; chaos; phase-space reconstruction; attractor;
D O I
10.1088/1361-6463/ad3374
中图分类号
O59 [应用物理学];
学科分类号
摘要
As a nonlinear dynamic system, the dynamic equation of triboelectric nanogenerator system is not only difficult to accurately establish, but also difficult to solve. The output signals of triboelectric nanogenerator system depends on the initial conditions of the system, which reflects the dynamic behavior of the system. Currently, there is little research on using the output signals to study the dynamic behavior of triboelectric nanogenerator system. Therefore, a dynamic simulation model of a freestanding triboelectric nanogenerator (F-TENG) system was established using COMSOL software. The mathematical model of the F-TENG system was fitted. Using chaos theory and its phase-space reconstruction technology, the phase-space trajectories of the F-TENG system were reconstructed through voltage signals under external factors, and the dynamic behavior of the F-TENG system was discussed and studied. Finally, validation experiments were carried out. The research shows that with the variation of internal factors and operating frequency, the mathematical model of the F-TENG system remains basically unchanged, and the variation law of output characteristics also remains basically unchanged. The F-TENG system is in periodic motion; with the variation of external factors such as resistance and friction layer spacing, the mathematical model of the F-TENG system will evolve in a complex direction, and the output characteristics will gradually distort. The F-TENG system will evolve from periodic motion to chaotic motion. The research results not only reveal the dynamic behavior and enrich the nonlinear dynamic theory of triboelectric nanogenerator system, but also provide theoretical guidance for increasing the working bandwidth and stability of triboelectric nanogenerator system.
引用
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页数:13
相关论文
共 16 条
[1]   Chaos in the fractionally damped broadband piezoelectric energy generator [J].
Cao, Junyi ;
Zhou, Shengxi ;
Inman, Daniel J. ;
Chen, Yangquan .
NONLINEAR DYNAMICS, 2015, 80 (04) :1705-1719
[2]   Chaotic characteristics and attractor evolution of friction noise during friction process [J].
Ding, Cong ;
Zhu, Hua ;
Sun, Guodong ;
Zhou, Yuankai ;
Zuo, Xue .
FRICTION, 2018, 6 (01) :47-61
[3]   Flexible triboelectric generator! [J].
Fan, Feng-Ru ;
Tian, Zhong-Qun ;
Wang, Zhong Lin .
NANO ENERGY, 2012, 1 (02) :328-334
[4]   Three-dimensional mathematical modelling and dynamic analysis of freestanding triboelectric nanogenerators [J].
Guo, Xin ;
Shao, Jiajia ;
Willatzen, Morten ;
Yang, Yi ;
Wang, Zhong Lin .
JOURNAL OF PHYSICS D-APPLIED PHYSICS, 2022, 55 (34)
[5]   Understanding and modeling of triboelectric-electret nanogenerator [J].
Hinchet, Ronan ;
Ghaffarinejad, Ali ;
Lu, Yingxian ;
Hasani, Javad Yavand ;
Kim, Sang-Woo ;
Basset, Philippe .
NANO ENERGY, 2018, 47 :401-409
[6]   Theoretical study on rotary-sliding disk triboelectric nanogenerators in contact and non-contact modes [J].
Jiang, Tao ;
Chen, Xiangyu ;
Yang, Keda ;
Han, Changbao ;
Tang, Wei ;
Wang, Zhong Lin .
NANO RESEARCH, 2016, 9 (04) :1057-1070
[7]   Segmentally Structured Disk Triboelectric Nanogenerator for Harvesting Rotational Mechanical Energy [J].
Lin, Long ;
Wang, Sihong ;
Xie, Yannan ;
Jing, Qingshen ;
Niu, Simiao ;
Hu, Youfan ;
Wang, Zhong Lin .
NANO LETTERS, 2013, 13 (06) :2916-2923
[8]  
Liu J X., 2023, Chin. J. Vib. Eng, V32, P1, DOI [10.19650/j.cnki.cjsi.2011.01.006, DOI 10.19650/J.CNKI.CJSI.2011.01.006]
[9]   A dynamics model of triboelectric nanogenerator transducers [J].
Liu Weiqi ;
Shi Jian .
NANO ENERGY, 2021, 89
[10]  
Luo Zhizeng, 2011, Chinese Journal of Scientific Instrument, V32, P33