用于加速爪蟾蝌蚪伤口愈合的等离子体源的表征*

K. Martus, Jashri Menon
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引用次数: 0

摘要

最近,等离子体射流在蝌蚪类非洲爪蟾(Xenopus laevis 1)伤口愈合中的应用。与未处理的对照组相比,将等离子体间接应用于蝌蚪的断尾产生了更快的生长速度,提高了细胞结构中的活性氧,并增加了再生蝌蚪的抗氧化酶。血浆暴露通过对细胞增殖和分化的影响,以及通过活性氧信号介导的血管生成,加速了伤口愈合和尾巴再生的动力学。放电源使用高纯度氦气,流速为50sccm,通过¼”石英管。铜电极附着在试管外表面距离试管末端5.0cm处。连接在电极上的是一个交流电源,工作频率为32kHz和12kV。该系统在一种制度下运行,使放电被限制在电极和管的出口孔径之间的流动区域。利用高分辨率光谱仪耦合CCD探测器测量了发射特征的轮廓。光谱分析表明,氮分子以中性态和电离态存在于管内。在300-315nm波长范围内观察到OH发射,并向石英管外延伸。利用第二正体系的发射谱线计算振动温度,结果为375±50K。在337nm处,将第二正体系跃迁拟合为玻尔兹曼分布,确定了旋转温度为375±50K。电流是通过监测与石英管出口孔相邻的金属板的接地连接,使用电流互感器来测量的。当系统没有等离子体供电时,信号由振幅小于0.5mA的正弦波组成,其频率与驱动电压(32kHz)相匹配。当等离子体“开启”时,信号由叠加在正弦波上的附加分量组成。附加分量是一个持续时间短(1 μs)的正电流脉冲(0.75mA),大约在高压达到最大值时出现。该电流脉冲的高度随着距离石英管出口孔径的距离而减小。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Charaterization Of A Plasma Source Used To Accelerate Wound Healing Of The Tadpole Xenopus Laevis*
A recent application of plasma jets has involved the healing of wounds in the tadpole species Xenopus laevis 1. The indirect application of the plasma to the amputated tail of the tadpole produced a faster rate of growth, elevated reactive oxygen species in the cellular structures, and an increase in antioxidant enzymes in the regenerate compared to that of the untreated control. The plasma exposure accelerated the dynamics of the wound healing and tail regeneration through its effects on cell proliferation and differentiation, as well as, angiogenesis mediated through reactive oxygen signaling. The discharge source operated with high purity Helium gas at a flow rate of 50sccm that passed through a ¼” quartz tube. A copper electrode was attached to the outer surface of the tube at a point 5.0cm from the end of the tube. Attached to the electrode was an AC power supply operating at 32kHz and 12kV. The system was operated in a regime such that the discharge was restricted to the flow region between the electrode and the exit aperture of the tube. The profiles of the emissions features were measured using a high-resolution spectrometer coupled to an CCD detector. The spectra indicated that molecular nitrogen was present within the tube in both the neutral and ionized states. OH emissions, in the wavelength region between 300–315nm, were observed inside the tube and extending outside of the quartz tube. The emission profile of the Second Positive Systems was used to calculate the vibrational temperature and it was found to be 375±50K. The rotational temperature was determined from a fitting of the Second Positive System transition at 337nm to a Boltzmann distribution and it was found to be 375±50K. The current was measured by monitoring the ground connection from a metal plate that was placed adjacent to the exit aperture of the quartz tube using a current transformer. When the system was powered without a plasma the signal consisted of a sinusoidal wave having an amplitude of less than 0.5mA at a frequency that matched the driving voltage (32kHz). When the plasma was “on” the signal consisted of an additional component superimposed on the sinusoidal wave. The additional component was a short duration (1 μs) positive current pulse (0.75mA) that appeared approximately at the time the high voltage reached its maximum value. The height of this current pulse decreased with distance from the exit aperture of the quartz tube.
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