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首页> 外文期刊>The European physical journal, D. Atomic, molecular, and optical physics >Experimental determination and numerical evaluation under simplifying assumptions of the ozone concentration in an atmospheric-pressure air DBD plasma
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Experimental determination and numerical evaluation under simplifying assumptions of the ozone concentration in an atmospheric-pressure air DBD plasma

机译:简化臭氧浓度在大气压空气DBD等离子体中的假设下的实验测定和数值评价

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In this work ozone concentration in a plane-to-plane Dielectric Barrier Discharge (DBD) reactor has been evaluated both experimentally and numerically. The reactor geometry has been chosen to generate a homogenous discharge. Therefore, simplified approaches for both experiments and numerical simulations have been utilized. The discharge was excited for 20 s in atmospheric-pressure quiescent air by means of a sinusoidal voltage of 15 kV peak at a frequency of 5 kHz in continuous operation. Electrical and optical measurements have been done to estimate the input parameters for the kinetics model. The ozone density within the discharge gap was measured by using the UV absorption method. The optical path travelled by the UV beam inside the reactor gap was estimated by means of Schlieren imaging. Within the time intervals and the dimensions considered, plasma was assumed to be uniform. This assumption was confirmed experimentally by iCCD images of the discharge. Numerical simulations have been performed by means of the zero-dimensional open-source code ZDPlasKin. A set of 622 reactions among 62 chemical species has been implemented, accounting for a 1% water vapour fraction. Reduced electric field, electron density and gas temperature were the input parameters of the code. Ozone density presented a production peak of about 1.3.10(17) cm(-3) half a second after discharge ignition. A steady state value of 6.10(16) cm(-3) was reached after a transient of about 12 s. Numerical simulation delivered ozone concentrations in good agreement with experimental data.
机译:在该工作中,在平面到平面介电屏障放电(DBD)反应器中的臭氧浓度已经通过实验和数值评估。已选择反应器几何体以产生均匀的放电。因此,已经利用了实验和数值模拟的简化方法。通过在连续操作中以5kHz的频率为5kV峰的正弦电压,在大气压静态空气中激发了20秒的电压20s。已经完成了电气和光学测量以估计动力学模型的输入参数。通过使用UV吸收方法测量放电间隙内的臭氧密度。通过Schlieren成像估计由电抗器间隙内部的UV光束行进的光路。在考虑的时间间隔内和尺寸内,假设等离子体是均匀的。通过DICCD图像实验确认该假设。通过零维开源ZdPlaskin执行了数值模拟。已经实施了62种化学物质中的一组622反应,占1%的水蒸气分数。电场降低,电子密度和气体温度是代码的输入参数。臭氧密度呈现出放电点火后约1.3.10(17)厘米(-3)半的生产峰值。在大约12秒的短暂后达到稳定状态值6.10(16)厘米(-3)。数值模拟与实验数据良好的一致交付臭氧浓度。

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