Investigations in the boron-carbon system with the aid of electron probe microanalysis

Karl A. Schwetz, P. Karduck
{"title":"Investigations in the boron-carbon system with the aid of electron probe microanalysis","authors":"Karl A. Schwetz,&nbsp;P. Karduck","doi":"10.1016/0022-5088(91)90345-5","DOIUrl":null,"url":null,"abstract":"<div><p>For boron carbide the limit of the homogeneity range at the carbon-rich side has not yet been firmly established. During the last 20 years carbon-rich limiting compositions have been reported corresponding to B<sub>43</sub>C (<em>i.e.</em> “B<sub>13</sub>C<sub>3</sub>”), B<sub>4.0</sub>C (i.e. “B<sub>12</sub>C<sub>3</sub>”) and B<sub>3.6</sub>C (<em>i.e.</em> “B<sub>11</sub>C<sub>3</sub>”). By means of quantitative electron probe microanalysis (EPMA) the composition of the boron carbide phase in the following samples has been determined: </p><ul><li><span>1.</span><span><p>(i) boron-carbon diffusion couples, prepared by hot isostatic pressing (HIP) of the pure elements at above 2000 °C;</p></span></li><li><span>2.</span><span><p>(ii) fused, regular boron carbide, obtained by carbothermic reduction of boric oxide at above 2500 °C (ESK electrofurnace process);</p></span></li><li><span>3.</span><span><p>(iii) dense boron carbide compacts made by pressureless sintering of carbothermic boron carbide powder or by HIP of magnesiothermic boron carbide powder at above 2000 °C.</p></span></li></ul><p>In each sample the carbon-rich limiting composition has been determined as B<sub>4.3</sub>C (18.8 at.% C) which corresponds to B<sub>13</sub>C<sub>2</sub>·C and is probably a solid solution of carbon in B<sub>13</sub>C<sub>2</sub>. The B<sub>12</sub>C<sub>3</sub> and B<sub>11</sub>C<sub>3</sub> compositions could not be found. For quantitative analysis a standard sample has been used, which was obtained by arc melting the pure elements with a <em>B</em>: <em>C</em> atomic ratio of 4.39. Also indirect <em>B</em>: <em>C</em> atomic ratio determinations via chemical analyses of crushed samples have produced evidence to support the limit 4.3 found by EPMA.</p></div>","PeriodicalId":17534,"journal":{"name":"Journal of The Less Common Metals","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"1991-09-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0022-5088(91)90345-5","citationCount":"60","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of The Less Common Metals","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0022508891903455","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 60

Abstract

For boron carbide the limit of the homogeneity range at the carbon-rich side has not yet been firmly established. During the last 20 years carbon-rich limiting compositions have been reported corresponding to B43C (i.e. “B13C3”), B4.0C (i.e. “B12C3”) and B3.6C (i.e. “B11C3”). By means of quantitative electron probe microanalysis (EPMA) the composition of the boron carbide phase in the following samples has been determined:

  • 1.

    (i) boron-carbon diffusion couples, prepared by hot isostatic pressing (HIP) of the pure elements at above 2000 °C;

  • 2.

    (ii) fused, regular boron carbide, obtained by carbothermic reduction of boric oxide at above 2500 °C (ESK electrofurnace process);

  • 3.

    (iii) dense boron carbide compacts made by pressureless sintering of carbothermic boron carbide powder or by HIP of magnesiothermic boron carbide powder at above 2000 °C.

In each sample the carbon-rich limiting composition has been determined as B4.3C (18.8 at.% C) which corresponds to B13C2·C and is probably a solid solution of carbon in B13C2. The B12C3 and B11C3 compositions could not be found. For quantitative analysis a standard sample has been used, which was obtained by arc melting the pure elements with a B: C atomic ratio of 4.39. Also indirect B: C atomic ratio determinations via chemical analyses of crushed samples have produced evidence to support the limit 4.3 found by EPMA.

电子探针微量分析对硼碳体系的研究
对于碳化硼,在富碳侧的均匀性范围的极限还没有确定。在过去的20年中,已经报道了与B43C(即“B13C3”)、B4.0C(即“B12C3”)和B3.6C(如“B11C3”)相对应的富碳极限成分。通过电子探针定量分析(EPMA)测定了以下样品中碳化硼相的组成:1.(i)硼-碳扩散偶,通过在2000°C以上对纯元素进行热等静压(HIP)制备;2.(ii)通过氧化硼在2500°C以上的碳热还原(ESK电铸工艺)获得的熔融规则碳化硼;3.(iii)通过碳热碳化硼粉末的无压烧结或在2000°C以上通过镁热碳化硼粉的HIP制备的致密碳化硼压块。在每个样品中,富碳极限组成被确定为B4.3C(18.8 at.%C),其对应于B13C2·C,并且可能是碳在B13C2中的固溶体。未发现B12C3和B11C3的组成。为了进行定量分析,使用了标准样品,该样品是通过电弧熔化B∶C原子比为4.39的纯元素而获得的。此外,通过对破碎样品的化学分析进行的间接B:C原子比测定也提供了支持EPMA发现的极限4.3的证据。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信