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电源频率和放电管长度是介质阻挡放电(DBD)臭氧产生的两个重要影响因素,在前期的研究基础上,采用合适的放电管长度和电源频率进行实验研究。实验研究了干空气源放电管长度、放电电压和气体流量对臭氧产生的影响,并进行了系统优化。研究结果表明:放电管长度由500 mm变为200 mm,在几乎不降低臭氧浓度下放电平均功率约降低了60%;臭氧浓度随放电电压和气体流量的增大先增大后降低;当流量为200 L/h、放电电压为2 698 V时,臭氧浓度与臭氧产率同时达到相对较高值,此时,臭氧浓度为5.3 g/m3时,臭氧产率为43.62 g/kWh。 相似文献
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为揭示混合放电臭氧高效发生的电能转换和传热机理,采用有限体积法数值求解质量、动量和能量守恒方程,实现对混合放电臭氧发生进行传热分析,并实验验证了该方法的可行性。研究结果表明:气体进入两放电间隙后温度逐渐升高,且两放电间隙温度相差较大,内放电空间平均温度比外放电空间平均温度平均高6.38 K;中心电极、内电介质、外介电质和外电极各部分内部径向温差较小;混合放电仅36.14%的电能转换为热能,其中气体从3根放电管中携带的热量分别为9.85%,7.39%和4.78%,气体经过3根放电管后最高温度仅为313.2 K。混合放电电能转化率高、气体温度相对较低,是一种非常有前途的臭氧发生形式。 相似文献
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The influence mechanism of a small amount of SF6 on ozone generation in oxygen or air discharge is investigated.Some results are obtained by probing into the number of the high-energy electrons,which have the sufficiency energy for generating ozone.Introducing a small amount of SF6 into oxygen sharply decreases the number of high-energy electrons,because the electron density decreases sharply while the mean electron energy remains constant due to higher breakdown voltage and lower discharge power,and some high-energy electrons are consumed by the excitation and attachment of SF6.In contrast,when a small amount of SF6 is added into dry air discharge,despite the consumption of the excitation and attachment of SF6,the number of high energy electrons increases sharply,which is attributed to the higher mean electron energy and electron density resulted from higher breakdown voltage and discharge power.When the volume fraction of SF6 increases from 0 to 2.22%,the ozone mass concentration and the ozone yield increase by 45.7% and 29.7%,respectively.Therefore,though the oxygen source should avoid the presence of SF6,adding a small amount of SF6 can improve the ozone mass concentration and the efficiency of ozone generation. 相似文献
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