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Ca_3Co_2O_6块体的放电等离子烧结及热电性能研究 被引量:1

Research on Spark Plasma Sintering and Thermoelectric Properties of Ca_3Co_2O_6 Bulk
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摘要 采用短时固相反应和放电等离子烧结(SR-SPS)方法,制备了单相多晶Ca3Co2O6陶瓷块,系统研究了制备条件及烧结工艺对Ca3Co2O6陶瓷块显微结构及热电性能的影响。研究表明,950℃下固相反应2h即能得到单相树枝状,尺寸约1~3μm的Ca3Co2O6粉末,延长焙烧时间虽然对物相影响不大,但会引起粉末颗粒长大,不利于SPS烧结;SPS烧结温度强烈影响着Ca3Co2O6陶瓷块的制备,本实验范围内,Ca3Co2O6陶瓷块体的最佳制备条件为950℃固相反应2h,SPS900℃保温5min,此时Ca3Co2O6陶瓷块具有P型半导体特性,电阻率ρ随温度的升高急剧下降,然后趋于平缓(高于600℃);Seebeck系数S随温度(100℃以上)升高稍有下降,热导率Ⅳ表现为先下降后增加,在500℃时仅为1.73W·m^-1·K^-1综合电性能与热性能结果,其无量纲因子ZT随 温度升高呈上升趋势,在本实验范围内,于700℃下达到最高值0.02。 Short-time solid reaction and spark plasma sintering method (SR-SPS) was used to prepare single-phase polycrystalline Ca3Co206 ceramic bulk, and effects of preparation condition and sintering technology were investigated in detail. Single-phase dendritic Ca3Co2O6 powders with grain size of about 1 - 3μm were obtained under 950 for 2 h by, solid-state reaction process, and prolonged reaction time could hardly influence phase structure, but it could make grain size growth, which is harmful for SPS sintering. Temperature of SPS strongly affects the preparation of Ca3Co2O6 ceramic bulk. In our experimental range, the best condition for Ca3Co206 ceramic bulk is to react under 950℃ for 2 h, and then sinter under 900℃ for 5 min by SPS. The bulk obtained by above technology shows character of p-type semiconductor, electrical resistivity ρ decrease sharply and then slightly, Seebeck coefficient S reduces, thermal conductivity r decreas- es and then increases with increasing temperature, the minimum value of r is 1.73 W- m- i. K^-1l at 500 ℃. As a result, the figureless factor of merit ZT shows in- creasing trend and the maximum value of ZT reaches 0.02 at 700 ℃ in our experimental range.
出处 《稀有金属》 EI CAS CSCD 北大核心 2006年第1期118-121,共4页 Chinese Journal of Rare Metals
基金 国家自然科学基金(50271001) 北京市教委科技发展重点资助项目(KZ200310005001) 国家发改委资助项目
关键词 Ca3Co2O6块体 放电等离子烧结 显微结构 热电性能 Ca3Co2O6 bulk SPS microstructure thermoelectric properties
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参考文献14

  • 1Sales B C,Mandrus D,Williams R K.Filled Skutterudite antimonides:A new class of thermoelectric materials[J].Science,1996,272:1325.
  • 2Nolas G S,Cohn J L,Slack G A.Effect of partial void filling on the lattice thermal conductivity of Skutterudites[J].Phys.Rev.B,1998,58:164.
  • 3Terasaki T,Sasago Y,Uchinokura K.Large thermoelectric power in NaCo2O4 single crystals[J].Phys.Rev.B.,1997,56(20):12685.
  • 4Funahashi R,Matsubara I,Ikuta H.An oxide single crystal with high thermoelectric performance in air[J].Jpn.J.Appl.Phys.,2000,39:L1127.
  • 5Tsubota T,Ohtaki M,Eguchi K.Transport properties and thermoelectric performance of (Zn1-yMgy)AlxO[J].J.Mater.Chem.,1998,8 (2):409.
  • 6Li S W,Funahashi R,Matsubara I,et al.High temperature thermoelectric properties of oxide Ca9Co12O28[J].J.Mater.Chem.,1999,9:1659.
  • 7Masset A C,Michel D,Maignan A,et al.Misfit-layered cobaltite with an anisotropic giant magnetoresistance:Ca3Co4O9[J].Phys.Rev.B.,2000,62(1):166.
  • 8Matsubara I,Funahashi R,Takeuchi T.Thermoelectric properties of spark plasma sintered Ca2.75Ga0.25Co4O9[J].J.Appl.Phys.,2001,90 (1):462.
  • 9Raquet B,Baibich M N,Broto J M,et al.Hopping conductivity in one-demensional Ca3Co2O6 single crystals[J].Phys.Rev.B.,2002,65:104442.
  • 10Mikami M,Funahashi R,Yoshimura M,et al.High-temperature thermoelectric properties of single-crystal Ca3Co2O6[J].Journal of Applied Physics,2003,94 (10):6579.

同被引文献11

  • 1聂长江,石友国,虞红春,周玉清,李建奇.Na_xCoO_2(0.75≤x≤1.0)中超结构的透射电镜研究[J].电子显微学报,2004,23(4):396-396. 被引量:1
  • 2Terasaki I,Sasago Y,Uchinokura K.Large thermoelectric power in NaCo2O4 single crystals[J].Physical Review B,1997,56(20):12685.
  • 3Takada K,Sakurai H,Takayama Muromachi E,Izumi F,Dilanian R A,Sasaki T.Superconductivity in two-dimensional CoO2 layers[J].Nature,2003,422:53.
  • 4Takada K,Sakurai H,Takayama Muromachi E,Izumi F,Dilanian R A,Sasaki T.Influences of interlayer distance and cobalt oxidation state on superconductivity of NaxCoO2[J].Physica C,2004,412-414:14.
  • 5Jorgensen J D,Avdeev M,Hinks D G,Burley J C,Short S.Crystal structure of the sodium cobaltate deuterate superconductor NaxCoO2·4xD2O(x≈1/3)[J].Physical Review B,2003,68(21):214517.
  • 6Sakurai H,Takada K,Sasaki T,Takayama Muromachi E.Characterization of superconductivity in NaxCoO2·yH2O[J].Physica C,2005,426-431:225.
  • 7Lynn J W,Huang Q,Brown C M,Miller V L,Foo M L,Schaak R E,Jones C Y,Mackey E A,Cava R J.Structure and dynamics of superconducting NaxCoO2 hydrate and its unhydrated analog[J].Physical Review B,2003,68(21):214516.
  • 8Badica P,Kondo T,Togano K.Critical current density and magnetic-field irreversibility of Na0.35CoO2·1.3H2O superconductor[J].Applied Physics Letters,2004,84(4):559.
  • 9Baskaran G.How ice enables superconductivity in NaxCoO2·yH2O by melting charge order:possibility of novel electric field effects[J].Physica C,2005,417:150.
  • 10Mochizuki M,Yanase Y,Ogata M.Ferromagnetic fluctuation and superconductivity in Na0.35CoO2·1.3H2O:FLEX study of multi-orbital Hubbard model[J].Physica B,2005,359-361:594.

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