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Electronic ground state OH(X) radical in a low-temperature atmospheric pressure plasma jet

机译:低温大气压等离子体射流中的电子基态OH(X)自由基

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摘要

The wide applicability of atmospheric pressure plasma jets in biomedicine stems from the presence of reactive nitrogen and oxygen species generated in these plasma jets. Knowing the absolute concentration of these reactive species is of utmost importance as it is critical, along with the particle flux obtained from the plasma feed gas flow rate to ensure that the correct dosage is applied during applications. In this study, we investigate and report the ground state OH(X) number density acquired using cavity ringdown spectroscopy, along the propagation axis (z-axis) of a cold atmospheric pressure helium plasma plume. The jet was generated by a repetitively pulsed mono-polar square wave of duration 1 μs running at a frequency of 9.9 kHz. The voltage supplied was 6.5 kV with the helium flow rate fixed at 3.6 standard liters per minute. The rotational and vibra-tional temperatures are simulated from the second positive system of nitrogen, N_2(C~3π_u - B~3π_g), with the rotational temperature being spatially constant at 300 K along the propagation axis of the atmospheric pressure plasma jet while the vibrational temperature is 3620 K at the beginning of the plume and is observed to decrease downstream. The 0H(A) emission intensity obtained via optical emission spectroscopy was observed to decrease downstream of the plasma jet. The OH(X) number density along the propagation axis was initially 2.2 ×10~(13) molecules cm"3 before increasing to a peak value of 2.4 × 10~(13) molecules cm~(-3), from which the number density was observed to decrease to 2.2 × 10~(13) molecules cm~(-3) downstream of the plasma jet. The total OH(A, X) in the plasma jet remained relatively constant along the propagation axis of the plasma jet before falling off at the tip of the jet. The increase in vibrational temperature downstream and the simultaneous measurements of both the excited state OH(A) and the ground state OH(X) reported in this study provide insights into the formation and consumption of this reactive oxygen species while also providing a reference for determining the radical number density dosage for future cold plasma irradiation studies.
机译:大气压等离子体射流在生物医学中的广泛应用源于这些等离子体射流中产生的反应性氮和氧物种的存在。知道这些反应性物质的绝对浓度至关重要,因为它与从血浆原料气流速获得的颗粒通量至关重要,以确保在使用过程中施加正确的剂量。在这项研究中,我们调查和报告使用腔衰荡光谱沿着冷大气压氦等离子体羽流的传播轴(z轴)获得的基态OH(X)数密度。射流是通过以9.9 kHz的频率运行的持续时间为1μs的重复脉冲单极性方波产生的。提供的电压为6.5 kV,氦气流速固定为每分钟3.6标准升。旋转温度和振动温度是根据第二个正氮系统N_2(C〜3π_u-B〜3π_g)进行模拟的,旋转温度沿大气压等离子体射流的传播轴在300 K处空间恒定,而羽流开始时的振动温度为3620 K,并且观察到下游温度降低。观察到通过光发射光谱法获得的0H(A)发射强度在等离子流的下游降低。沿传播轴的OH(X)数密度最初为2.2×10〜(13)分子cm·(3),然后增加到峰值为2.4×10〜(13)分子cm·(-3)。等离子体射流下游的密度降低到2.2×10〜(13)cm〜(-3)分子,沿射流的传播轴,等离子体射流中的总OH(A,X)保持相对恒定。这项研究报告了下游振动温度的升高以及对激发态OH(A)和基态OH(X)的同时测量,从而提供了对该反应物的形成和消耗的见解。氧物种,同时也为确定未来冷等离子体辐射研究的自由基数密度剂量提供了参考。

著录项

  • 来源
    《Journal of Applied Physics 》 |2016年第16期| 163303.1-163303.11| 共11页
  • 作者单位

    Department of Physics and Astronomy, Mississippi State University, Starkville, Mississippi 39759, USA;

    Department of Physics and Astronomy, Mississippi State University, Starkville, Mississippi 39759, USA;

    Department of Physics and Astronomy, Mississippi State University, Starkville, Mississippi 39759, USA;

    Department of Physics and Astronomy, Mississippi State University, Starkville, Mississippi 39759, USA;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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