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Formation studies and controlled production of carbon nanohorns using continuous in situ characterization techniques

机译:使用连续原位表征技术的碳纳米角的形成研究和受控生产

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摘要

The formation of carbon nanohorns by laser ablation was investigated using a scanning differential mobility analyzer combined with an ultrafine condensation particle counter. The measurement technique provided time-resolved size distributions for the carbon nanoparticles every minute during the course of the production run. The instrument performance was reasonably stable most of the time; however, during laser ablation, shockwave oscillations leading to significant transient flow and pressure variations were shown to disrupt the DMAs ability to measure accurate distributions. On the basis of the general trend observed in the data taken during the laser-ablation experiments, we found that the geometric mean diameter of the produced population shifted to larger particle sizes with increases in pulse width. For a given laser peak power and repetition rate, carbon nanoparticles of mobility diameter close to 100 nm were produced in a large abundance using longer laser pulse lengths ( e. g., 10 ms) as compared to the shorter pulse lengths ( e. g., 1 ms). A quantitative assessment of the particle size dispersion ( using statistics like the geometric standard deviation) in relation to the laser pulse width could not be done with certainty as the shockwave disturbances produced by the laser-ablation process caused significant disruption to SMPS measurements. When laser ablation was not in operation, it was found that carbon nanoparticles with mobility diameters centred at about 20 nm could be produced by thermally desorbing the previously deposited carbon nanoparticles from the reactor wall at temperatures greater than 1300 K.
机译:使用扫描差动迁移率分析仪结合超细凝聚粒子计数器研究了通过激光烧蚀形成碳纳米角。在生产过程中,测量技术每分钟提供一次碳纳米颗粒的时间分辨尺寸分布。大部分时间里仪器的性能都相当稳定。但是,在激光烧蚀过程中,冲击波振荡导致明显的瞬态流量和压力变化,显示出破坏了DMA测量准确分布的能力。根据在激光烧蚀实验中获得的数据中观察到的总体趋势,我们发现,随着脉冲宽度的增加,所产生的总体的几何平均直径向更大的颗粒尺寸转移。对于给定的激光峰值功率和重复率,与较短的脉冲长度(例如1ms)相比,使用较长的激光脉冲长度(例如10ms)以大的丰度产生迁移率直径接近100nm的碳纳米颗粒。由于激光烧蚀过程产生的冲击波干扰严重干扰了SMPS测量,因此无法确定地对粒度分布的定量评估(使用诸如几何标准偏差之类的统计数据)相对于激光脉冲宽度的评估。当不进行激光烧蚀时,发现可以通过在高于1300 K的温度下从反应器壁上热脱附先前沉积的碳纳米颗粒来生产迁移率直径集中在约20 nm的碳纳米颗粒。

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