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Effects of Acoustic Modulation and Mixed Fuel on Flame Synthesis of Carbon Nanomaterials in an Atmospheric Environment

机译:大气环境中声调制和混合燃料对碳纳米材料火焰合成的影响

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摘要

In this study, methane–ethylene jet diffusion flames modulated by acoustic excitation in an atmospheric environment were used to investigate the effects of acoustic excitation frequency and mixed fuel on nanomaterial formation. Acoustic output power was maintained at a constant value of 10 W, while the acoustic excitation frequency was varied (f = 0–90 Hz). The results show that the flame could not be stabilized on the port when the ethylene volume concentration (ΩE) was less than 40% at f = 10 Hz, or when ΩE = 0% (i.e., pure methane) at f = 90 Hz. The reason for this is that the flame had a low intensity and was extinguished by the entrained air due to acoustic modulation. Without acoustic excitation (f = 0 Hz), the flame was comprised of a single-layer structure for all values of ΩE, and almost no carbon nanomaterials were synthesized. However, with acoustic excitation, a double-layer flame structure was generated for frequencies close to both the natural flickering frequency and the acoustically resonant frequency. This double-layer flame structure provided a favorable flame environment for the fabrication of carbon nanomaterials. Consequently, the synthesis of carbon nano-onions was significantly enhanced by acoustic excitation near both the natural flickering frequency and the acoustically resonant frequency. At f = 20 Hz (near the natural flickering frequency) for 0% ≤ ΩE ≤ 100%, a quantity of carbon nano-onions (CNOs) piled like bunches of grapes was obtained as a result of improved mixing of the fuel with ambient air. High-density CNOs were also produced at f = 70 Hz (close to the acoustically resonant frequency) for 40% ≤ ΩE ≤ 100%. Furthermore, carbon nanotubes (CNTs) were synthesized only at 80 Hz for ΩE = 0%. The suitable temperature range for the synthesis of CNTs was slightly higher than that for the formation of CNOs (about 600 °C for CNTs; 510–600 °C for CNOs).
机译:在这项研究中,在大气环境中通过声激发调制的甲烷-乙烯射流扩散火焰用于研究声激发频率和混合燃料对纳米材料形成的影响。声输出功率保持在10 W的恒定值,而声激励频率则有所变化(f = 0–90 Hz)。结果表明,当乙烯体积浓度(ΩE)在f = 10 Hz时小于40%,或在f = 90 Hz时ΩE= 0%(即纯甲烷)时,火焰无法在端口上稳定。其原因是火焰强度低,并且由于声学调制而被夹带的空气熄灭。没有声激发(f = 0 Hz),火焰由所有ΩE值的单层结构组成,几乎没有碳纳米材料被合成。然而,通过声激发,对于接近于自然闪烁频率和声共振频率的频率,产生了双层火焰结构。这种双层火焰结构为碳纳米材料的制造提供了有利的火焰环境。因此,通过在自然闪烁频率和声学共振频率附近的声激发,碳纳米洋葱的合成得到了显着增强。对于0%≤ΩE≤100%,在f = 20 Hz(接近自然闪烁频率)时,由于改善了燃料与环境空气的混合,因此获得了像葡萄串一样堆积的碳纳米洋葱(CNO)数量。 。在40%≤ΩE≤100%的情况下,还以f = 70 Hz(接近声共振频率)产生了高密度CNO。此外,碳纳米管(CNTs)仅在80 Hz下合成,ΩE= 0%。碳纳米管合成的合适温度范围略高于CNO的形成温度范围(CNT约为600°C; CNO约为5​​10–600°C)。

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