Synthesis of branched carbon nanotubes from coal
Synthesis of branched carbon nanotubes from coal
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DOI:
10.1016/j.carbon.2005.12.030
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发表时间:
2006-06
期刊:
影响因子:
10.9
通讯作者:
Zhiyu Wang;Zongbin Zhao;J. Qiu
中科院分区:
文献类型:
--
作者:
Zhiyu Wang;Zongbin Zhao;J. Qiu
Carbon nanotubes with Y-or T-type junction morphologies have attracted much attention because of the application potential in 2-D or 3-D nanodevice with novel properties [1–3] and in fiber-reinforced composites [4]. The intermolecular or branched structures intrinsically imbedded into the straight tube stems may lead to significant changes in electronic and mechanical properties of the tubes [5]. After the first report about Y-junction carbon nanotubes in 1995 [6], several methods including arc-discharge [6], alumina template [7], catalytic hydrocarbon decomposition [8–10] and hot-filament CVD method [4] have been developed with an aim of making branched carbon nanotubes (BCNTs) in large quantity. In comparison to other methods available now, the arc-discharge approach is still widely used because of its simplicity and convenience in operation and the capability of producing tubes with well-developed graphene-based structures. Here we report the synthesis of BCNTs from coal, the cheapest natural carbon source, by arc-discharge with copper as catalyst. It has been found that BCNTs with a purity of ca. 70% can be obtained in large quantity under suitable experimental conditions.The preparation experiments were carried out in helium in a traditional DC arc-discharge reactor. The anode was a high-purity graphite tube (10 mm outside diameter, 8 mm inside diameter and 150 mm in length) filled with a mixture of anthracite coal (from Yunnan Province, China) and CuO powder (smaller than 150 μm in size) while the cathode was a high purity graphite rod (15 mm outside diameter, 30 mm in length). The analysis data of coal is shown in Table 1. During the arcing process, the cathode remained the same before and after the arc discharge. The weight ratio of CuO powder to coal powder in the mixture for filling the anode tube was 3: 7. For each run that normally lasted about 10 min, the arc discharge was conducted with DC current of 70–80 A and voltage of 25–30 V in helium at