Loading…
Comparative study on diffuse dielectric barrier discharges excited by unipolar positive versus bipolar pulses in atmospheric air
Diffuse discharges excited by unipolar positive and bipolar pulses can be achieved by a self-designed dielectric barrier discharge (DBD) structure (a metal rod is inserted into a traditional parallel-plate DBD structure) exposed in airflow. For a self-designed DBD excited by unipolar positive pulses...
Saved in:
Published in: | Journal of applied physics 2019-04, Vol.125 (16) |
---|---|
Main Authors: | , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
cited_by | cdi_FETCH-LOGICAL-c327t-1e6ebe6f8dbb44092f437eb750f312f43483c956fff29d3883935af83a74316e3 |
---|---|
cites | cdi_FETCH-LOGICAL-c327t-1e6ebe6f8dbb44092f437eb750f312f43483c956fff29d3883935af83a74316e3 |
container_end_page | |
container_issue | 16 |
container_start_page | |
container_title | Journal of applied physics |
container_volume | 125 |
creator | Guo, Hongfei Wang, YuYing Xu, Yongfeng Fan, Zhihui Ren, Chunsheng |
description | Diffuse discharges excited by unipolar positive and bipolar pulses can be achieved by a self-designed dielectric barrier discharge (DBD) structure (a metal rod is inserted into a traditional parallel-plate DBD structure) exposed in airflow. For a self-designed DBD excited by unipolar positive pulses, only a primary discharge occurs in a voltage pulse. When the applied voltage is low, a diffuse discharge first appears near the anode. As the voltage further increases, a diffuse discharge appears in a larger area near the anode. Until the applied voltage is high enough, the discharge fills the whole discharge gap. Additionally, there is a priority region around the metal rod for the development of a diffuse discharge. However, for a self-designed DBD excited by bipolar pulses, two separate discharges are observed in a voltage pulse. The primary discharge occurs at the rising front of the voltage pulse, and the secondary discharge (reverse discharge) takes place at the falling front of the voltage pulse. When the applied voltage is low, the diffuse discharge first starts from the priority region around the metal rod placed in the center of the discharge electrode. As the voltage further increases, the diffuse discharge appears in a larger area around the metal rod. The above observations about the different spatial evolutions of diffuse discharge areas excited by unipolar positive and bipolar pulses are mainly ascribed to the difference of a strong local electric field caused by residual charges. This diffuse discharge has potential applications in surface treatment of materials and thin film deposition. |
doi_str_mv | 10.1063/1.5085456 |
format | article |
fullrecord | <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_journals_2212249853</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2212249853</sourcerecordid><originalsourceid>FETCH-LOGICAL-c327t-1e6ebe6f8dbb44092f437eb750f312f43483c956fff29d3883935af83a74316e3</originalsourceid><addsrcrecordid>eNqdkE9PwzAMxSMEEmNw4BtE4gRSIWmaNjmiiX_SJC5wjtLWYUFbU5x2Yjc-Ohkb4s7J8vPPz_Ij5Jyza85KccOvJVOykOUBmXCmdFZJyQ7JhLGcZ0pX-picxPjOGOdK6An5moVVb9EOfg00DmO7oaGjrXdujJAqLKEZ0De0togeMEmxWVh8g0jhs_EDtLTe0LHzfVhapH2I_sdrDRjHSOtffVzGtOI7aodViP0CtqbW4yk5cjbNzvZ1Sl7v715mj9n8-eFpdjvPGpFXQ8ahhBpKp9q6Lgqmc1eICupKMif4timUaLQsnXO5boVKzwlpnRK2KgQvQUzJxc63x_AxQhzMexixSydNnvM8L7SSIlGXO6rBECOCMz36lcWN4cxsAzbc7ANO7NWOjSmGFGDo_gevA_6Bpm-d-Aasc4wH</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2212249853</pqid></control><display><type>article</type><title>Comparative study on diffuse dielectric barrier discharges excited by unipolar positive versus bipolar pulses in atmospheric air</title><source>American Institute of Physics:Jisc Collections:Transitional Journals Agreement 2021-23 (Reading list)</source><creator>Guo, Hongfei ; Wang, YuYing ; Xu, Yongfeng ; Fan, Zhihui ; Ren, Chunsheng</creator><creatorcontrib>Guo, Hongfei ; Wang, YuYing ; Xu, Yongfeng ; Fan, Zhihui ; Ren, Chunsheng</creatorcontrib><description>Diffuse discharges excited by unipolar positive and bipolar pulses can be achieved by a self-designed dielectric barrier discharge (DBD) structure (a metal rod is inserted into a traditional parallel-plate DBD structure) exposed in airflow. For a self-designed DBD excited by unipolar positive pulses, only a primary discharge occurs in a voltage pulse. When the applied voltage is low, a diffuse discharge first appears near the anode. As the voltage further increases, a diffuse discharge appears in a larger area near the anode. Until the applied voltage is high enough, the discharge fills the whole discharge gap. Additionally, there is a priority region around the metal rod for the development of a diffuse discharge. However, for a self-designed DBD excited by bipolar pulses, two separate discharges are observed in a voltage pulse. The primary discharge occurs at the rising front of the voltage pulse, and the secondary discharge (reverse discharge) takes place at the falling front of the voltage pulse. When the applied voltage is low, the diffuse discharge first starts from the priority region around the metal rod placed in the center of the discharge electrode. As the voltage further increases, the diffuse discharge appears in a larger area around the metal rod. The above observations about the different spatial evolutions of diffuse discharge areas excited by unipolar positive and bipolar pulses are mainly ascribed to the difference of a strong local electric field caused by residual charges. This diffuse discharge has potential applications in surface treatment of materials and thin film deposition.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.5085456</identifier><identifier>CODEN: JAPIAU</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Air flow ; Anodes ; Applied physics ; Comparative studies ; Dielectric barrier discharge ; Electric fields ; Electric potential ; Plasma ; Plates (structural members) ; Surface treatment ; Thin films</subject><ispartof>Journal of applied physics, 2019-04, Vol.125 (16)</ispartof><rights>Author(s)</rights><rights>2019 Author(s). Published under license by AIP Publishing.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c327t-1e6ebe6f8dbb44092f437eb750f312f43483c956fff29d3883935af83a74316e3</citedby><cites>FETCH-LOGICAL-c327t-1e6ebe6f8dbb44092f437eb750f312f43483c956fff29d3883935af83a74316e3</cites><orcidid>0000-0002-1283-7006 ; 0000-0003-1617-4198</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Guo, Hongfei</creatorcontrib><creatorcontrib>Wang, YuYing</creatorcontrib><creatorcontrib>Xu, Yongfeng</creatorcontrib><creatorcontrib>Fan, Zhihui</creatorcontrib><creatorcontrib>Ren, Chunsheng</creatorcontrib><title>Comparative study on diffuse dielectric barrier discharges excited by unipolar positive versus bipolar pulses in atmospheric air</title><title>Journal of applied physics</title><description>Diffuse discharges excited by unipolar positive and bipolar pulses can be achieved by a self-designed dielectric barrier discharge (DBD) structure (a metal rod is inserted into a traditional parallel-plate DBD structure) exposed in airflow. For a self-designed DBD excited by unipolar positive pulses, only a primary discharge occurs in a voltage pulse. When the applied voltage is low, a diffuse discharge first appears near the anode. As the voltage further increases, a diffuse discharge appears in a larger area near the anode. Until the applied voltage is high enough, the discharge fills the whole discharge gap. Additionally, there is a priority region around the metal rod for the development of a diffuse discharge. However, for a self-designed DBD excited by bipolar pulses, two separate discharges are observed in a voltage pulse. The primary discharge occurs at the rising front of the voltage pulse, and the secondary discharge (reverse discharge) takes place at the falling front of the voltage pulse. When the applied voltage is low, the diffuse discharge first starts from the priority region around the metal rod placed in the center of the discharge electrode. As the voltage further increases, the diffuse discharge appears in a larger area around the metal rod. The above observations about the different spatial evolutions of diffuse discharge areas excited by unipolar positive and bipolar pulses are mainly ascribed to the difference of a strong local electric field caused by residual charges. This diffuse discharge has potential applications in surface treatment of materials and thin film deposition.</description><subject>Air flow</subject><subject>Anodes</subject><subject>Applied physics</subject><subject>Comparative studies</subject><subject>Dielectric barrier discharge</subject><subject>Electric fields</subject><subject>Electric potential</subject><subject>Plasma</subject><subject>Plates (structural members)</subject><subject>Surface treatment</subject><subject>Thin films</subject><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNqdkE9PwzAMxSMEEmNw4BtE4gRSIWmaNjmiiX_SJC5wjtLWYUFbU5x2Yjc-Ohkb4s7J8vPPz_Ij5Jyza85KccOvJVOykOUBmXCmdFZJyQ7JhLGcZ0pX-picxPjOGOdK6An5moVVb9EOfg00DmO7oaGjrXdujJAqLKEZ0De0togeMEmxWVh8g0jhs_EDtLTe0LHzfVhapH2I_sdrDRjHSOtffVzGtOI7aodViP0CtqbW4yk5cjbNzvZ1Sl7v715mj9n8-eFpdjvPGpFXQ8ahhBpKp9q6Lgqmc1eICupKMif4timUaLQsnXO5boVKzwlpnRK2KgQvQUzJxc63x_AxQhzMexixSydNnvM8L7SSIlGXO6rBECOCMz36lcWN4cxsAzbc7ANO7NWOjSmGFGDo_gevA_6Bpm-d-Aasc4wH</recordid><startdate>20190428</startdate><enddate>20190428</enddate><creator>Guo, Hongfei</creator><creator>Wang, YuYing</creator><creator>Xu, Yongfeng</creator><creator>Fan, Zhihui</creator><creator>Ren, Chunsheng</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-1283-7006</orcidid><orcidid>https://orcid.org/0000-0003-1617-4198</orcidid></search><sort><creationdate>20190428</creationdate><title>Comparative study on diffuse dielectric barrier discharges excited by unipolar positive versus bipolar pulses in atmospheric air</title><author>Guo, Hongfei ; Wang, YuYing ; Xu, Yongfeng ; Fan, Zhihui ; Ren, Chunsheng</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c327t-1e6ebe6f8dbb44092f437eb750f312f43483c956fff29d3883935af83a74316e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Air flow</topic><topic>Anodes</topic><topic>Applied physics</topic><topic>Comparative studies</topic><topic>Dielectric barrier discharge</topic><topic>Electric fields</topic><topic>Electric potential</topic><topic>Plasma</topic><topic>Plates (structural members)</topic><topic>Surface treatment</topic><topic>Thin films</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Guo, Hongfei</creatorcontrib><creatorcontrib>Wang, YuYing</creatorcontrib><creatorcontrib>Xu, Yongfeng</creatorcontrib><creatorcontrib>Fan, Zhihui</creatorcontrib><creatorcontrib>Ren, Chunsheng</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Guo, Hongfei</au><au>Wang, YuYing</au><au>Xu, Yongfeng</au><au>Fan, Zhihui</au><au>Ren, Chunsheng</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Comparative study on diffuse dielectric barrier discharges excited by unipolar positive versus bipolar pulses in atmospheric air</atitle><jtitle>Journal of applied physics</jtitle><date>2019-04-28</date><risdate>2019</risdate><volume>125</volume><issue>16</issue><issn>0021-8979</issn><eissn>1089-7550</eissn><coden>JAPIAU</coden><abstract>Diffuse discharges excited by unipolar positive and bipolar pulses can be achieved by a self-designed dielectric barrier discharge (DBD) structure (a metal rod is inserted into a traditional parallel-plate DBD structure) exposed in airflow. For a self-designed DBD excited by unipolar positive pulses, only a primary discharge occurs in a voltage pulse. When the applied voltage is low, a diffuse discharge first appears near the anode. As the voltage further increases, a diffuse discharge appears in a larger area near the anode. Until the applied voltage is high enough, the discharge fills the whole discharge gap. Additionally, there is a priority region around the metal rod for the development of a diffuse discharge. However, for a self-designed DBD excited by bipolar pulses, two separate discharges are observed in a voltage pulse. The primary discharge occurs at the rising front of the voltage pulse, and the secondary discharge (reverse discharge) takes place at the falling front of the voltage pulse. When the applied voltage is low, the diffuse discharge first starts from the priority region around the metal rod placed in the center of the discharge electrode. As the voltage further increases, the diffuse discharge appears in a larger area around the metal rod. The above observations about the different spatial evolutions of diffuse discharge areas excited by unipolar positive and bipolar pulses are mainly ascribed to the difference of a strong local electric field caused by residual charges. This diffuse discharge has potential applications in surface treatment of materials and thin film deposition.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.5085456</doi><tpages>11</tpages><orcidid>https://orcid.org/0000-0002-1283-7006</orcidid><orcidid>https://orcid.org/0000-0003-1617-4198</orcidid></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0021-8979 |
ispartof | Journal of applied physics, 2019-04, Vol.125 (16) |
issn | 0021-8979 1089-7550 |
language | eng |
recordid | cdi_proquest_journals_2212249853 |
source | American Institute of Physics:Jisc Collections:Transitional Journals Agreement 2021-23 (Reading list) |
subjects | Air flow Anodes Applied physics Comparative studies Dielectric barrier discharge Electric fields Electric potential Plasma Plates (structural members) Surface treatment Thin films |
title | Comparative study on diffuse dielectric barrier discharges excited by unipolar positive versus bipolar pulses in atmospheric air |
url | http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-06T19%3A02%3A42IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Comparative%20study%20on%20diffuse%20dielectric%20barrier%20discharges%20excited%20by%20unipolar%20positive%20versus%20bipolar%20pulses%20in%20atmospheric%20air&rft.jtitle=Journal%20of%20applied%20physics&rft.au=Guo,%20Hongfei&rft.date=2019-04-28&rft.volume=125&rft.issue=16&rft.issn=0021-8979&rft.eissn=1089-7550&rft.coden=JAPIAU&rft_id=info:doi/10.1063/1.5085456&rft_dat=%3Cproquest_cross%3E2212249853%3C/proquest_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c327t-1e6ebe6f8dbb44092f437eb750f312f43483c956fff29d3883935af83a74316e3%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=2212249853&rft_id=info:pmid/&rfr_iscdi=true |