Surface charge deposition inside a capillary glass tube by an atmospheric pressure discharge in air
This paper presents simulations of the dynamics of surface charging by an air plasma discharge at atmospheric pressure initiated by a needle anode inside a capillary glass tube. During the discharge propagation in the tube, the highest positive surface charge density is observed close to the point e...
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Veröffentlicht in: | European physical journal. Applied physics 2011-07, Vol.55 (1), p.13810 |
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description | This paper presents simulations of the dynamics of surface charging by an air plasma discharge at atmospheric pressure initiated by a needle anode inside a capillary glass tube. During the discharge propagation in the tube, the highest positive surface charge density is observed close to the point electrode. We have shown that during the discharge propagation, the positive surface charge is increasing behind the discharge front, while the electric field at the surface is decreasing. Then, we have studied the influence of the tube radius, its permittivity and the applied pulsed voltage on surface charges. We have shown that the surface charge density during the discharge propagation is inversely proportional to the tube radius and surface charge densities of 30–50 nC/cm2 for a tube with Rtube = 100 μm and an applied voltage of 12 kV have been obtained. We have also noted that a higher permittivity results in a higher surface charge density and a faster surface charge deposition. Then we have shown that the surface charge deposited is proportional to the applied voltage. Finally, at the end of the voltage pulse, our simulations indicate that the positive surface charge deposited during the discharge propagation in the tube decreases to very low values in few nanoseconds. |
doi_str_mv | 10.1051/epjap/2011100504 |
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During the discharge propagation in the tube, the highest positive surface charge density is observed close to the point electrode. We have shown that during the discharge propagation, the positive surface charge is increasing behind the discharge front, while the electric field at the surface is decreasing. Then, we have studied the influence of the tube radius, its permittivity and the applied pulsed voltage on surface charges. We have shown that the surface charge density during the discharge propagation is inversely proportional to the tube radius and surface charge densities of 30–50 nC/cm2 for a tube with Rtube = 100 μm and an applied voltage of 12 kV have been obtained. We have also noted that a higher permittivity results in a higher surface charge density and a faster surface charge deposition. Then we have shown that the surface charge deposited is proportional to the applied voltage. Finally, at the end of the voltage pulse, our simulations indicate that the positive surface charge deposited during the discharge propagation in the tube decreases to very low values in few nanoseconds.</description><identifier>ISSN: 1286-0042</identifier><identifier>EISSN: 1286-0050</identifier><identifier>DOI: 10.1051/epjap/2011100504</identifier><language>eng</language><publisher>Les Ulis: EDP Sciences</publisher><subject>Physics</subject><ispartof>European physical journal. 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Applied physics</title><description>This paper presents simulations of the dynamics of surface charging by an air plasma discharge at atmospheric pressure initiated by a needle anode inside a capillary glass tube. During the discharge propagation in the tube, the highest positive surface charge density is observed close to the point electrode. We have shown that during the discharge propagation, the positive surface charge is increasing behind the discharge front, while the electric field at the surface is decreasing. Then, we have studied the influence of the tube radius, its permittivity and the applied pulsed voltage on surface charges. We have shown that the surface charge density during the discharge propagation is inversely proportional to the tube radius and surface charge densities of 30–50 nC/cm2 for a tube with Rtube = 100 μm and an applied voltage of 12 kV have been obtained. We have also noted that a higher permittivity results in a higher surface charge density and a faster surface charge deposition. Then we have shown that the surface charge deposited is proportional to the applied voltage. Finally, at the end of the voltage pulse, our simulations indicate that the positive surface charge deposited during the discharge propagation in the tube decreases to very low values in few nanoseconds.</description><subject>Physics</subject><issn>1286-0042</issn><issn>1286-0050</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNpFkDFPwzAQhSMEEqWwM1psDKF3SRM7Y6mAIioxAILNurhO65ImwU4Q_fe4pCrTvTt99_T0guAS4QYhwZFu1tSMIkBEgATGR8EAI5GGu-X4oMfRaXDm3BoAMBXJIFAvnS1IaaZWZJeaLXRTO9OaumKmcmahGTFFjSlLslu2LMk51na5ZvmWUcWo3dSuWWlrFGusdq6z3sO4vZvxhLHnwUlBpdMX-zkM3u7vXqezcP788DidzEMVi3EbagU8yxLMixgjEl5BAZgQz4hy4gXPYp1GixQ5j7xQEanc31GkOqKEKB4G173vikrZWLPxkWVNRs4mc7m7AXDMBI6_0bNXPdvY-qvTrpXrurOVjyczEGnMBY89BD2kbO2c1cXBFUHuWpd_rcv_1v1L2L8Y1-qfA0_2U6Y85okU8C5vnz7m_RL_AseLhNI</recordid><startdate>201107</startdate><enddate>201107</enddate><creator>Jánský, J.</creator><creator>Bourdon, A.</creator><general>EDP Sciences</general><scope>BSCLL</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope><scope>1XC</scope><scope>VOOES</scope><orcidid>https://orcid.org/0000-0003-3662-4651</orcidid></search><sort><creationdate>201107</creationdate><title>Surface charge deposition inside a capillary glass tube by an atmospheric pressure discharge in air</title><author>Jánský, J. ; Bourdon, A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c384t-ec079951bf312a89510f015a79aaba7f793e62d61772e62c2acbba7186e2a5aa3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Jánský, J.</creatorcontrib><creatorcontrib>Bourdon, A.</creatorcontrib><collection>Istex</collection><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Hyper Article en Ligne (HAL)</collection><collection>Hyper Article en Ligne (HAL) (Open Access)</collection><jtitle>European physical journal. Applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Jánský, J.</au><au>Bourdon, A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Surface charge deposition inside a capillary glass tube by an atmospheric pressure discharge in air</atitle><jtitle>European physical journal. Applied physics</jtitle><date>2011-07</date><risdate>2011</risdate><volume>55</volume><issue>1</issue><spage>13810</spage><pages>13810-</pages><issn>1286-0042</issn><eissn>1286-0050</eissn><abstract>This paper presents simulations of the dynamics of surface charging by an air plasma discharge at atmospheric pressure initiated by a needle anode inside a capillary glass tube. During the discharge propagation in the tube, the highest positive surface charge density is observed close to the point electrode. We have shown that during the discharge propagation, the positive surface charge is increasing behind the discharge front, while the electric field at the surface is decreasing. Then, we have studied the influence of the tube radius, its permittivity and the applied pulsed voltage on surface charges. We have shown that the surface charge density during the discharge propagation is inversely proportional to the tube radius and surface charge densities of 30–50 nC/cm2 for a tube with Rtube = 100 μm and an applied voltage of 12 kV have been obtained. We have also noted that a higher permittivity results in a higher surface charge density and a faster surface charge deposition. Then we have shown that the surface charge deposited is proportional to the applied voltage. Finally, at the end of the voltage pulse, our simulations indicate that the positive surface charge deposited during the discharge propagation in the tube decreases to very low values in few nanoseconds.</abstract><cop>Les Ulis</cop><pub>EDP Sciences</pub><doi>10.1051/epjap/2011100504</doi><orcidid>https://orcid.org/0000-0003-3662-4651</orcidid><oa>free_for_read</oa></addata></record> |
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source | Bacon EDP Sciences France Licence nationale-ISTEX-PS-Journals-PFISTEX; EDP Sciences |
subjects | Physics |
title | Surface charge deposition inside a capillary glass tube by an atmospheric pressure discharge in air |
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