Effects of the transverse electric field on nanosecond pulsed dielectric barrier discharge in atmospheric airflow

Yongfeng XU (徐永锋); Hongfei GUO (郭宏飞); Yuying WANG (王玉英); Zhihui FAN (樊智慧); Chunsheng REN (任春生)

doi:10.1088/2058-6272/ab6530

Plasma Science and Technology > 2020 > 22(5): 55403-055403. > DOI: 10.1088/2058-6272/ab6530

Yongfeng XU (徐永锋), Hongfei GUO (郭宏飞), Yuying WANG (王玉英), Zhihui FAN (樊智慧), Chunsheng REN (任春生). Effects of the transverse electric field on nanosecond pulsed dielectric barrier discharge in atmospheric airflow[J]. Plasma Science and Technology, 2020, 22(5): 55403-055403. DOI: 10.1088/2058-6272/ab6530

Citation:

PDF (2565 KB)

Effects of the transverse electric field on nanosecond pulsed dielectric barrier discharge in atmospheric airflow

Funds: This work is supported by National Natural Science Foundation of China (No. 51437002).

More Information

Received Date: July 24, 2019
Revised Date: December 18, 2019
Accepted Date: December 22, 2019

Graphical Abstract

Abstract

Abstract

In this paper, an asymmetric electrode geometry (the misalignment between the ends of highvoltage and grounded electrodes) is proposed in order to investigate the effects of the transverse electric field on nanosecond pulsed dielectric barrier discharge (DBD). The results show that diffuse discharge manifests in the misaligned region and the micro-discharge channel in the aligned region moves directionally. Moreover, the diffuse discharge area increases with the decrease of the discharge gap and pulse repetition frequency, which is consistent with the variation of the moving velocity of the micro-discharge channel. When airflow is introduced into the discharge gap in the same direction as the transverse electric field, the dense filamentary discharge region at the airflow inlet of asymmetric electrode geometry is larger than that of symmetric electrode geometry. However, when the direction of the airflow is opposite to that of the transverse electric field, the dense filamentary discharge region of asymmetric electrode geometry is reduced. The above phenomena are mainly attributed to the redistribution of the space charges induced by the transverse electric field.
- dielectric barrier discharge,
- high-voltage,
- atmospheric pressure air,
- airflow,
- lowtemperatureplasma,
- nanosecond pulsed discharge

FullText(HTML)

References (50)

References

[1]	Kogelschatz U 2003 Plasma Chem. Plasma Process 23 1
[2]	Ono R and Oda T 2007 J. Phys. D: Appl. Phys. 40 176
[3]	Ognier S et al 2009 Plasma Chem. Plasma Process. 29 261
[4]	Shao T et al 2017 IEEE Trans. Dielectr. Electr. Insul. 24 1557
[5]	Boeuf J P 2003 J. Phys. D: Appl. Phys. 36 R53
[6]	Jiang H et al 2011 IEEE Trans. Plasma Sci. 39 2076
[7]	Williamson J M et al 2006 J. Phys. D: Appl. Phys. 39 4400
[8]	Shao T et al 2008 J. Phys. D: Appl. Phys. 41 215203
[9]	Ito T et al 2010 J. Phys. D: Appl. Phys. 43 062001
[10]	Takaki K et al 2005 Appl. Phys. Lett. 86 151501
[11]	Palmer A J 1974 Appl. Phys. Lett. 25 138
[12]	Guo H F et al 2018 Phys. Plasmas 25 093505
[13]	Duan X X et al 2009 Phys. Rev. E 80 016202
[14]	Xu S W, Li L L and Ouyang J T 2015 Plasma Sci. Technol.17 384
[15]	Abolmasov S N, Shirafuji T and Tachibana K 2005 IEEE Trans. Plasma Sci. 33 941
[16]	Pavon S et al 2007 J. Phys. D: Appl. Phys. 40 1733
[17]	Chirokov A et al 2004 Plasma Sources Sci. Technol. 13 623
[18]	Okazaki S et al 1993 J. Phys. D: Appl. Phys. 26 889
[19]	Golubovskii Y B et al 2004 J. Phys. D: Appl. Phys. 37 1346
[20]	Wang X X et al 2006 Plasma Sources Sci. Technol. 15 845
[21]	Liu W Z et al 2017 EPL 118 45001
[22]	Stollenwerk L et al 2006 Phys. Rev. Lett. 96 255001
[23]	Ye Q Z et al 2013 Plasma Sci. Technol. 15 1112
[24]	Panousis E et al 2009 IEEE Trans. Plasma Sci. 37 1004
[25]	Liu Y D et al 2016 Phys. Plasmas 23 113508
[26]	Yu S et al 2016 Phys. Plasmas 23 023510
[27]	Lee H W et al 2010 Plasma Processes Polym. 7 274
[28]	Ohtsu Y and Nagamatsu K 2018 Jpn. J. Appl. Phys. 57 01AB01
[29]	Akishev Y et al 2011 Plasma Sources Sci. Technol. 20 024005
[30]	Kogelschatz U 2010 J. Phys.: Conf. Ser. 257 012015
[31]	Fridman A, Chirokov A and Gutsol A 2005 J. Phys. D: Appl.Phys. 38 R1
[32]	Eliasson B and Kogelschatz U 1991 IEEE Trans. Plasma Sci.19 309
[33]	Eliasson B, Hirth M and Kogelschatz U 1987 J. Phys. D: Appl.Phys. 20 1421
[34]	Kozlov K V et al 2001 J. Phys. D: Appl. Phys. 34 3164
[35]	Song H M et al 2016 Chin. Phys. B 25 035204
[36]	Wu Y et al 2010 Chin. J. Aeronaut. 23 39
[37]	Wu Y et al 2008 Appl. Phys. Lett. 93 031503
[38]	Liu Y D et al 2018 Phys. Plasmas 25 033519
[39]	Luo S Q, Denning M and Scharer J E 2008 J. Appl. Phys. 104 013301
[40]	Laux C O et al 2003 Plasma Sources Sci. Technol. 12 125
[41]	Yu L et al 2001 Plasma Chem. Plasma Process. 21 483
[42]	Tang J, Duan Y X and Zhao W 2010 Appl. Phys. Lett. 96 191503
[43]	Bayoda K D, Benard N and Moreau E 2015 J. Appl. Phys. 118 063301
[44]	Shao T et al 2006 J. Phys. D: Appl. Phys. 39 2192
[45]	Liu Y D et al 2017 Phys. Plasmas 24 113514
[46]	Moss R S, Eden J G and Kushner M J 2004 J. Phys. D: Appl.Phys. 37 2502
[47]	Qi H C et al 2016 Plasma Sci. Technol. 18 520
[48]	Huang X J et al 2011 Phys. Plasmas 18 033503
[49]	Fan Z H et al 2016 Phys. Plasmas 23 123520
[50]	Fan Z H et al 2019 IEEE Trans. Plasma Sci. 47 4312

[1]	Jingwen FAN, Huijie YAN, Ting LI, Yurong MAO, Jiaqi LI, Jian SONG. Surface charge characteristics in a three-electrode surface dielectric barrier discharge[J]. Plasma Science and Technology, 2024, 26(11): 115403. DOI: 10.1088/2058-6272/ad7821
[2]	Victor F TARASENKO, Dmitry V BELOPLOTOV, Alexei N PANCHENKO, Dmitry A SOROKIN. Formation of diffuse and spark discharges between two needle electrodes with the scattering of particles[J]. Plasma Science and Technology, 2024, 26(9): 094003. DOI: 10.1088/2058-6272/ad34aa
[3]	Ronggang WANG (王荣刚), Qizheng JI (季启政), Tongkai ZHANG (张桐恺), Qing XIA (夏清), Yu ZHANG (张宇), Jiting OUYANG (欧阳吉庭). Discharge characteristics of a needle-to-plate electrode at a micro-scale gap[J]. Plasma Science and Technology, 2018, 20(5): 54017-054017. DOI: 10.1088/2058-6272/aaa436
[4]	Xuebao LI (李学宝), Dayong LI (李大勇), Qian ZHANG (张迁), Yinfei LI (李隐飞), Xiang CUI (崔翔), Tiebing LU (卢铁兵). The detailed characteristics of positive corona current pulses in the line-to-plane electrodes[J]. Plasma Science and Technology, 2018, 20(5): 54014-054014. DOI: 10.1088/2058-6272/aaa66b
[5]	Donglai WANG (王东来), Tiebing LU (卢铁兵), Yuan WANG (王源), Bo CHEN (陈博), Xuebao LI (李学宝). Measurement of surface charges on the dielectric film based on field mills under the HVDC corona wire[J]. Plasma Science and Technology, 2018, 20(5): 54008-054008. DOI: 10.1088/2058-6272/aaac26
[6]	Cheng PAN (潘成), Ju TANG (唐炬), Dibo WANG (王邸博), Yi LUO (罗毅), Ran ZHUO (卓然), Mingli FU (傅明利). Decay characters of charges on an insulator surface after different types of discharge[J]. Plasma Science and Technology, 2017, 19(7): 75503-075503. DOI: 10.1088/2058-6272/aa6436
[7]	WANG Yanhui (王艳辉), YE Huanhuan (叶换换), ZHANG Jiao (张佼), WANG Qi (王奇), ZHANG Jie (张杰), WANG Dezhen (王德真). Numerical Study of Pulsed Dielectric Barrier Discharge at Atmospheric Pressure Under the Needle-Plate Electrode Configuration[J]. Plasma Science and Technology, 2016, 18(5): 478-484. DOI: 10.1088/1009-0630/18/5/06
[8]	H. Z. ALISOY, S. ALAGOZ, G. T. ALISOY, B. B. ALAGOZ. An Investigation of Ionic Flows in a Sphere-Plate Electrode Gap[J]. Plasma Science and Technology, 2013, 15(10): 1012-1019. DOI: 10.1088/1009-0630/15/10/10
[9]	MA Hailiang (马海亮), DONG Baogguo (董保国), YAN Yuliang (闫玉良). Microscopic Effective Charges and the B(E2) Values of Terminating States in Mirror Nuclei ⁵¹Mn and ⁵¹Fe[J]. Plasma Science and Technology, 2012, 14(7): 603-606. DOI: 10.1088/1009-0630/14/7/08
[10]	HAO Lixia, WANG Wei, ZHAN Huamao, HAN Xiaohui, DENG Lihong. Effect of space charge on the propagation path of air gap discharge[J]. Plasma Science and Technology, 2011, 13(6): 714-718.