CN103178202A - 新型热电转换材料及其制备方法,以及使用该热电转换材料的热电转换器件 - Google Patents
新型热电转换材料及其制备方法,以及使用该热电转换材料的热电转换器件 Download PDFInfo
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Abstract
本发明公开了一种由下面的化学式表示的新型热电转换材料:Bi1-xCu1-yO1-zTe。在上面的化学式1中:0≤x<1,0≤y<1,0≤z<1且x+y+z>0。使用该热电转换材料的热电转换器件具有优异的能量转换效率。
Description
本申请是申请日为2009年8月31日,申请号为200980108016.1,发明名称为“新型热电转换材料及其制备方法,以及使用该热电转换材料的热电转换器件”的发明专利申请(国际申请号:PCT/KR2009/004883)的分案申请。
技术领域
本发明涉及一种热电转换材料及其制备方法,以及使用该热电转换材料的热电转换器件。
背景技术
热电转换器件被用于热电发电和热电制冷等。例如,热电发电是一种发电方式,其使用由在热电转换器件中的温度差异导致的温差电动势将热能转换为电能。
热电转换器件的能量转换效率取决于热电转换材料的塞贝克系数、电导率和热导率。更具体地说,热电转换材料的能量转换效率与塞贝克系数的平方和电导率成正比,且与热导率成反比。因此,需要开发出具有高塞贝克系数或高电导率或低热导率的热电转换材料以改进热电转换器件的能量转换效率。
发明内容
本发明的一个目的是提供一种具有优异热电转换性能的热电转换材料。
本发明的另一目的是提供一种制备所述热电转换材料的方法。
本发明的再一个目的是提供一种使用所述热电转换材料的热电转换器件。
在对热电转换材料进行反复研究后,本发明人成功合成了由以下化学式1表示的化合物半导体。并且,本发明人发现了此化合物可以用作热电转换器件的热电转换材料,并完成了本发明。
<化学式1>
Bi1-xCu1-yO1-zTe
其中0≤x<1,0≤y<1,0≤z<1且x+y+z>0。
在化学式1中,x、y和z分别优选为0≤x≤0.5、0≤y≤0.5和0≤z≤0.5,更分别优选为0≤x≤0.2、0≤y≤0.2和0≤z≤0.2。
本发明还提供了一种通过混合Bi2O3、Bi、Cu和Te的各个粉末并烧结该混合材料而制备由以上化学式1表示的所述热电转换材料的方法。
在本发明的制备方法中,烧结温度优选为400~570℃。
有益效果
根据本发明的热电转换材料具有优异的热电转换性能,且由此其可以取代常规热电转换材料或者与常规的热电转换材料一起有效应用于热电转换器件。
附图说明
附图说明了本发明的优选实施方式,并与本发明的详细说明一起用于进一步理解本发明的实质,因此,本发明不应解释为仅限于在附图中所示的内容。
图1是通过比较X射线衍射图与结构模型的理论图谱说明BiCuOTe的Rietveld精修图谱的图。
图2是说明BiCuOTe的晶体结构的图。
图3是说明根据本发明的实施例2、4和6的化合物的X射线衍射图的图。
图4是说明根据本发明的实施例1和2的化合物以及根据对比实施例的化合物的功率因数的图。
图5是说明根据本发明的实施例3~5的化合物以及根据对比实施例的化合物的功率因数的图。
图6是说明根据本发明的实施例1、2和6的化合物以及根据对比实施例的化合物的功率因数的图。
具体实施方式
根据本发明的热电转换材料由以下化学式1表示。
<化学式1>
Bi1-xCu1-yO1-zTe
其中0≤x<1,0≤y<1,0≤z<1且x+y+z>0。
在化学式1中,x、y和z分别优选为0≤x≤0.5、0≤y≤0.5和0≤z≤0.5,更分别优选为0≤x≤0.2、0≤y≤0.2和0≤z≤0.2。
换言之,根据本发明的热电转换材料的特征在于,在BiCuOTe中,Bi、Cu和O中的至少一种是相对缺位的。具体地说,在仅Bi缺位的情况下,在上述化学式1中的x、y和z可以分别为0<x≤0.1、y=0和z=0。在仅Cu缺位的情况下,x、y和z可以分别为x=0、0<y≤0.2和z=0。在Bi和O都缺位的情况下,x、y和z可以分别为0<x≤0.1、y=0和0<z≤0.1。
如上所述,塞贝克系数和电导率越高且热导率越低,热电转换性能就越高。虽然下文中将给出说明,但是BiCuOTe具有超晶格结构,其中Cu2Te2层和Bi2O2层沿c晶轴重复排列,因此其具有比Bi2Te3(一种常规商用热电转换材料)显著更低的热导率,并具有与Bi2Te3相似或比Bi2Te3更高的塞贝克系数。因此,BiCuOTe作为热电转换材料是非常有用的。然而,BiCuOTe具有相对较低的电导率。为了改进其电导率,它需要增加载流子(即空穴)的浓度。在本发明中,载流子浓度的增加是通过Bi、Cu和O中的至少一种元素的相对缺位来实现的。
因此,根据本发明的热电转换材料是一种新型材料,其不同于常规的热电转换材料。根据本发明的热电转换材料具有优异的热电转换性能,且由此其可以取代常规热电转换材料或者与常规的热电转换材料一起有效应用于热电转换器件。
上述化学式1的热电转换材料可以通过混合Bi2O3、Bi、Cu和Te的各个粉末并烧结该混合材料来制备,但本发明并不限于此。
根据本发明的化合物半导体可以通过在真空中烧结或通过在流动气体(如部分包括氢或不包括氢的Ar、He或N2)中烧结来制备。烧结温度优选为约400~750℃,更优选为400~570℃。
同时,虽然上述描述是以根据本发明的热电转换材料中的Te以化学计量上固定的量使用为基础进行描述的,但是Te可由另一种元素(如S、Se、As、Sb等)部分替代。这种情况遵循本发明的如下构想:Bi、Cu和O中的至少一种元素的部分缺位引起载流子浓度的增加,导致热电转换性能的改进。因此,应当解释为本发明的范围覆盖了除了具有部分缺位的元素以外的一种元素被另一种元素取代的情况。
以下,将参考以下实施例详述本发明。然而,本发明的实施例可以以不同方式修改和改变,且本发明的范围不应解释为限于以下实施例。本发明提供的实施例是为了使本领域的技术人员更全面地理解本发明。
<对比实施例>
BiCuOTe的合成
首先,为合成BiCuOTe,使用玛瑙研钵充分混合1.1198g的Bi2O3(Aldrich,99.9%,100目)、0.5022g的Bi(Aldrich,99.99%,<10m)、0.4581g的Cu(Aldrich,99.7%,3m)和0.9199g的Te(Aldrich,99.99%,约100目)。将混合的材料放入石英管中,真空密封并在510℃加热15小时,从而得到BiCuOTe粉末。
为进行X射线衍射分析,将测试部分充分粉碎,置于X射线衍射分析仪(Bruker D8-Advance XRD)的试样夹上,并通过扫描进行测量,其中,扫描间隔为0.02度,使用射线照射,施加电压为50KV且施加电流为40mA。
使用TOPAS程序(R.W.Cheary,A.Coelho,J.Appl.Crystallogr.25(1992)109-121;Bruker AXS,TOPAS3,Karlsruhe,Germany(2000))分析得到的材料的晶体结构,且分析结果示于下表1和图2中。
原子 | 位置 | x | y | z | 占有率 | Beq |
Bi | 2c | 0.25 | 0.25 | 0.37257(5) | 1 | 0.56(1) |
Cu | 2a | 0.75 | 0.25 | 0 | 1 | 0.98(3) |
O | 2b | 0.75 | 0.25 | 0.5 | 1 | 0.26(12) |
Te | 2c | 0.25 | 0.25 | 0.81945(7) | 1 | 0.35(1) |
图1是通过比较X射线衍射图与结构模型的理论图谱说明BiCuOTe的Rietveld精修图谱的图。参考图1,可以发现测得的图谱与根据表1的结果计算的图谱是一致的。因此,根据对比实施例得到的材料被鉴定为BiCuOTe。
如图2所示,BiCuOTe化合物半导体显示出天然超晶格结构,其中,Cu2Te2层和Bi2O2层沿c晶轴重复排列。
<实施例1和2>
Bi
1-x
CuOTe的合成:
除了为了使BiCuOTe中的Bi部分缺位,根据下表2控制各种原料粉末的混合量以外,以与对比实施例相同的方式合成Bi1-xCuOTe。用于合成的各种原料粉末的混合量如下(单位:g)。
表2
类别 | Bi2O3 | Bi | Cu | Te |
实施例1(x=0.01) | 1.6881 | 0.7344 | 0.6907 | 1.3868 |
实施例2(x=0.04) | 1.7141 | 0.6765 | 0.7013 | 1.4082 |
<实施例3~5>
BiCu
1-y
OTe的合成:
除了为了使BiCuOTe中的Cu部分缺位,根据下表3控制各种原料粉末的混合量以外,以与对比实施例相同的方式合成BiCu1-yOTe。用于合成的各种原料粉末的混合量如下(单位:g)。
表3
类别 | Bi2O3 | Bi | Cu | Te |
实施例3(y=0.01) | 1.6822 | 0.7545 | 0.6814 | 1.3820 |
实施例4(y=0.04) | 1.6900 | 0.7579 | 0.6638 | 1.3884 |
实施例5(y=0.1) | 1.7057 | 0.7650 | 0.6281 | 1.4013 |
<实施例6>
Bi0.96CuO0.94Te的合成
除了相对减少Bi2O3的混合量以使Bi和O都部分缺位以外,以与对比实施例相同的方式合成Bi0.96CuO0.94Te。用于合成的各种原料粉末的混合量如下(单位:g)。
表4
类别 | Bi2O3 | Bi | Cu | Te |
实施例6 | 1.6150 | 0.7706 | 0.7029 | 1.4115 |
而且,根据实施例2、4和6的化合物的测试部分以与对比实施例中相同的方式制备,并进行X射线衍射分析,且对各个材料进行鉴别,如图3所示。
<热电转换性能的评价>
将根据上述对比实施例和实施例得到的各个测试部分模压成直径为4mm且长度为15mm的圆柱体。使用CIP(冷等静压机)对该圆柱体施加200Mpa的压力。随后,将得到的产物放在石英管中在510℃下真空烧结10小时。
使用ZEM-2(Ulvac-Rico公司)在预定温度间隔下测量各个烧结的测试部分的电导率和塞贝克系数。计算出功率因数,其用于指示热电转换性能,且其被定义为塞贝克系数的平方与电导率的乘积。计算出的功率因数示于图4~6中。
参考图4~6,可以发现根据实施例1~6的热电转换材料与对比实施例的BiCuOTe相比具有显著改进的功率因数,因此根据本发明的热电转换材料具有优异的热电转换性能。
Claims (18)
1.具有天然超晶格结构的热电转换材料BiCuOTe,其中Cu2Te2层和Bi2O2层沿c晶轴交替排列,
其中,BiCuOTe的Bi、Cu和O中的至少一种是相对缺位的。
2.根据权利要求1所述的热电转换材料,
其中,当x、y和z各自为所述缺位的比例时,x、y和z分别为0≤x≤0.5、0≤y≤0.5和0≤z≤0.5,且x+y+z>0。
3.根据权利要求2所述的热电转换材料,
其中,所述x、y和z分别为0≤x≤0.2、0≤y≤0.2和0≤z≤0.2。
4.根据权利要求3所述的热电转换材料,
其中,所述x、y和z分别为0<x≤0.1、y=0和z=0。
5.根据权利要求3所述的热电转换材料,
其中,所述x、y和z分别为x=0、0<y≤0.2和z=0。
6.根据权利要求3所述的热电转换材料,
其中,所述x、y和z分别为0<x≤0.1、y=0和0<z≤0.1。
7.一种制备权利要求1中所述的热电转换材料的方法,该方法包括:
混合Bi2O3、Bi、Cu和Te的各个粉末;以及
烧结该混合材料以制备所述热电转换材料,
其中,所述烧结温度为400~750℃。
8.根据权利要求7所述的制备热电转换材料的方法,
其中,所述烧结温度为400~570℃。
9.一种热电转换器件,其包括权利要求1~6中任一项所述的热电转换材料。
10.具有天然超晶格结构的热电转换材料BiCuOTe,其中BiTeCu层和O层沿c晶轴交替排列,
其中,BiCuOTe的Bi、Cu和O中的至少一种是相对缺位的。
11.根据权利要求10所述的热电转换材料,
其中,当x、y和z各自为所述缺位的比例时,x、y和z分别为0≤x≤0.5、0≤y≤0.5和0≤z≤0.5,且x+y+z>0。
12.根据权利要求11所述的热电转换材料,
其中,所述x、y和z分别为0≤x≤0.2、0≤y≤0.2和0≤z≤0.2。
13.根据权利要求12所述的热电转换材料,
其中,所述x、y和z分别为0<x≤0.1、y=0和z=0。
14.根据权利要求12所述的热电转换材料,
其中,所述x、y和z分别为x=0、0<y≤0.2和z=0。
15.根据权利要求12所述的热电转换材料,
其中,所述x、y和z分别为0<x≤0.1、y=0和0<z≤0.1。
16.一种制备权利要求10中所述的热电转换材料的方法,该方法包括:
混合Bi2O3、Bi、Cu和Te的各个粉末;以及
烧结该混合材料以制备所述热电转换材料,
其中,所述烧结温度为400~750℃。
17.根据权利要求16所述的制备热电转换材料的方法,
其中,所述烧结温度为400~570℃。
18.一种热电转换器件,其包括权利要求10~15中任一项所述的热电转换材料。
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