Flexible Thermoelectric Polymers and Systems. Группа авторов. Читать онлайн. Newlib. NEWLIB.NET

Автор: Группа авторов
Издательство: John Wiley & Sons Limited
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Жанр произведения: Физика
Год издания: 0
isbn: 9781119550631
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      Names: Ouyang, Jianyong, author.

      Title: Flexible thermoelectric polymers and systems / edited by Jianyong Ouyang, National University of Singapore.

      Description: 1st edition. | Hoboken, NJ : Wiley, 2022. | Includes index.

      Identifiers: LCCN 2021033949 (print) | LCCN 2021033950 (ebook) | ISBN 9781119550709 (hardback) | ISBN 9781119550723 (ebook) | ISBN 9781119550686 (epdf) | ISBN 9781119550631 (epub)

      Subjects: LCSH: Thermoelectric apparatus and appliances–Materials. | Thermoresponsive polymers. | Flexible electronics.

      Classification: LCC TK2950 .O987 2022 (print) | LCC TK2950 (ebook) | DDC 621.31/243–dc23

      LC record available at https://lccn.loc.gov/2021033949 LC ebook record available at https://lccn.loc.gov/2021033950

      Cover Design: Wiley

      Cover Image: © Ajwad Creative/Getty

      List of Contributors

      Shanshan Chen School of Energy & Power Engineering State Key Laboratory of Power Transmission Equipment & System Security and New Technology Chongqing University Chongqing P. R. China

      Xinyi Chen Key Laboratory of Textile Science & Technology of Ministry of Education College of Textiles Donghua University Shanghai China

      Hanlin Cheng Department of Materials Science and Engineering National University of Singapore Singapore Singapore

      Ming Hui Chua Institute of Materials Research and Engineering (IMRE) Agency for Science, Research and Technology (A*STAR) Singapore Singapore

      Minzhi Du Key Laboratory of Textile Science & Technology of Ministry of Education College of Textiles Donghua University Shanghai China

      Zeng Fan School of Physics Dalian University of Technology Dalian P. R. China

      Xue Han Key Laboratory of Textile Science & Technology of Ministry of Education College of Textiles Donghua University Shanghai China

      Fengxing Jiang Flexible Electronics Innovation Institute Jiangxi Science and Technology Normal University Nanchang P. R. China Department of Physics Jiangxi Science and Technology Normal University Nanchang P. R. China

      Yuanyuan Jing Key Laboratory of Textile Science & Technology of Ministry of Education College of Textiles Donghua University Shanghai China

      Meng Li MOE Key Laboratory of Low‐grade Energy Utilization Technologies and Systems CQU‐NUS Renewable Energy Materials & Devices Joint Laboratory School of Energy & Power Engineering Chongqing University Chongqing P. R. China

      Zaifang Li China‐Australia Institute for Advanced Materials and Manufacturing Jiaxing University Jiaxing P. R. China

      Peipei Liu Department of Physics Jiangxi Science and Technology Normal University Nanchang P. R. China

      Congcong Liu Flexible Electronics Innovation Institute Jiangxi Science and Technology Normal University Nanchang P. R. China

      Yang Liu MOE Key Laboratory of Low‐grade Energy Utilization Technologies and Systems CQU‐NUS Renewable Energy Materials & Devices Joint Laboratory School of Energy & Power Engineering Chongqing University Chongqing P. R. China

      Baoyang Lu Flexible Electronics Innovation Institute Jiangxi Science and Technology Normal University Nanchang P. R. China

      Jianyong Ouyang Department of Materials Science and Engineering National University of Singapore Singapore Singapore

      Lujun Pan School of Physics Dalian University of Technology Dalian P. R. China

      Yue Shu MOE Key Laboratory of Low‐grade Energy Utilization Technologies and Systems CQU‐NUS Renewable Energy Materials & Devices Joint Laboratory School of Energy & Power Engineering Chongqing University Chongqing P. R. China

      Kuan Sun MOE Key Laboratory of Low‐grade Energy Utilization Technologies and Systems CQU‐NUS Renewable Energy Materials & Devices Joint Laboratory School of Energy & Power Engineering Chongqing University Chongqing P. R. China

      Ady Suwardi Institute of Materials Research and Engineering (IMRE) Agency for Science, Research and Technology (A*STAR) Singapore Singapore

      Zhenghong Xiong MOE Key Laboratory of Low‐grade Energy Utilization Technologies and Systems CQU‐NUS Renewable Energy Materials & Devices Joint Laboratory School of Energy & Power Engineering Chongqing University Chongqing P. R. China

      Jianwei Xu Institute of Materials Research and Engineering (IMRE) Agency for Science, Research and Technology (A*STAR) Singapore Singapore

      Jingkun Xu Flexible Electronics Innovation Institute Jiangxi Science and Technology Normal University Nanchang P. R. China

      Yuanyuan Zheng Key Laboratory of Textile Science & Technology of Ministry of Education College of Textiles, Donghua University Shanghai China

      Yujie Zheng School of Energy & Power Engineering State Key Laboratory of Power Transmission Equipment & System Security and New Technology Chongqing University Chongqing P. R. China

      Fengling Zhang Department of Physics Chemistry and Biology Linköping University Linköping, Sweden

      Kun Zhang Key Laboratory of Textile Science & Technology of Ministry of Education College of Textiles Donghua University Shanghai China

      Yinhua Zhou Wuhan National Laboratory for Optoelectronics, and School of Optical and Electronic Information Huazhong University of Science and Technology Wuhan Hubei China

      Yongli Zhou MOE Key Laboratory of Low‐grade Energy Utilization Technologies and Systems CQU‐NUS Renewable Energy Materials & Devices Joint Laboratory School of Energy & Power Engineering Chongqing University Chongqing P. R. China

      Preface

      Thermoelectric materials are interesting because they can be used to directly convert heat into electricity. Some conductive materials can exhibit a notable voltage under temperature gradient, that is, the Seebeck effect. The thermovoltage with respect to the temperature is called Seebeck voltage. The Seebeck voltage can be positive or negative depending on the accumulation of the charge carrier(s) at the two ends under temperature gradient. A p‐type thermoelectric material exhibits a positive Seebeck voltage, while an n‐type thermoelectric material has a negative Seebeck voltage. High Seebeck coefficient has been observed on semiconductors and semimetals. The value is related to the relative position of the Fermi level from the top of the valence band or the bottom of the conduction band or simply the doping level since a change in the doping level can shift the Fermi level. Apart from the Seebeck coefficient, a high electrical conductivity is also required for efficient thermoelectric conversion. However, a good thermoelectric material should have a low thermal conductivity so that more heat can be utilized for power generation. Thermoelectric