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Study On Performance Optimization Of Bi2Te2.7Se0.3 Thermoelectric Materials

Posted on:2021-04-16Degree:MasterType:Thesis
Country:ChinaCandidate:X ChenFull Text:PDF
GTID:2381330626466206Subject:Materials Science and Engineering
Abstract/Summary:PDF Full Text Request
Thermoelectric?TE?materials have a wide application prospect in the field of power generation and solid refrigeration,because it can convert thermal energy to electric energy directly and reversely based on Seebeck effect and Peltier effect.Bi2Te3-based alloys are the most typical thermoelectric material used near room temperature and have been put into commercial application.However,compaered to high-performance p-type Bi2Te3-based alloys,n-type Bi2Te3 has lower TE performance.How to effectively improve TE performance of n-type Bi2Te3 is the key to achieve wide application for Bi2Te3-based TE materials.The n-type Bi2Te2.7Se0.3 is selected as research object in this paper.The main research contents and obtained conclusions are as following:?1?Due to the small band gap?about 0.15 eV?of Bi2Te3,the intrinsic excitation occurring near room temperature causes that its TE performance decreases sharply with increasing temperature.In this paper,Bi2Te2.7Se0.3 with excess Te are prepared by an energy-saving and time-saving method?high-energy ball milling method and DC rapid hot pressing?,and the intrinsic point defects are adjusted by controlling Te content.Excess Te atoms occupy Bi sites to form positively charged antisite defect Te·Bi,which significantly increases the carrier concentration,thereby enhancing the electrical conductivity and delaying the intrinsic excitation.Because the intrinsic excitation is effectively delayed,the bipolar thermal conductivity decreases significantly.In addition,the antisite defect Te·Bi enhances the phonon scattering,thereby reducing the lattice thermal conductivity.Finally,the ZT peak of Bi2Te2.71Se0.3 reaches 0.9 at 373 K,and the average ZT reaches 0.82 between 300 K and 498 K,which is 20%and 61%higher than that of Bi2Te2.7Se0.3,respectively,indicating its application potential in TE power generation?below 500 K?.?2?The commercial Bi2Te2.7Se0.3 is selected as the matrix material,and the Bi2Te2.7Se0.3/Bi2S3 heterostructure is constructed in situ using an ion exchange reaction.The sulfur-containing group?-CS-?is first adsorbed on the surface of Bi2Te2.7Se0.3 powder particles,and then hydrolyzed in situ to form S2-ions.Under the solvothermal condition,anion exchange reaction occurs with Bi2Te2.7Se0.3 to form Bi2S3.Bi2Te2.7Se0.3/Bi2S3 hetero-interface with appropriate concentration has no significant effect on the electrical conductivity.And the Seebeck coefficient is enhanced due to the potential barrier filering effect of the hetero-interface,which improves the power factor to a certain extent.In addition,the Bi2Te2.7Se0.3/Bi2S3 hetero interface significantly enhances phonon scattering,thereby effectively reducing the lattice thermal conductivity.Finally,the maximum ZT reaches 0.7 at 473 K,and the average ZT value reaches 0.61 between 300 K and 498 K,which is 23%and 25%higher than the matrix,respectively.?3?After commercial Bi2Te2.7Se0.3 and S powder are uniformly mixed at a certain ratio,the mixed powder is subjected to DC rapid hot-pressing sintering.During the high-temperature solidification process,part of the S is sublimated,leaving nano-scale pores in the material,and the other part of the S is doped into the Bi2Te2.7Se0.3 lattice to form point defects in atomic-scale.The electrical conductivity is slightly decreased because of the introducing of defects.However,the Seebeck coefficient is significantly enhanced due to the improvement of the effective mass,thereby improving the power factor.In addition,multi-scale defects significantly enhance phonon scattering,thereby effectively reducing lattice thermal conductivity.Finally,the ZT value reaches 0.85 at 473 K,and the average ZT value reaches 0.74 between 300 K and 548 K,which is 49%and 51%higher than the matrix,respectively.
Keywords/Search Tags:Bi2Te2.7Se0.3, intrinsic point defects, heterostructure, multi-scale defects, thermoelectric properties
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