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DC Field | Value | Language |
---|---|---|
dc.contributor.author | Saeed, A. | - |
dc.contributor.author | Khan, A. W. | - |
dc.contributor.author | Shafiq, M. | - |
dc.contributor.author | Jan, F. | - |
dc.contributor.author | Abrar, M. | - |
dc.contributor.author | Zaka-Ul-Islam, M. | - |
dc.contributor.author | Zakaullah, M. | - |
dc.date.accessioned | 2019-12-04T09:40:28Z | - |
dc.date.available | 2019-12-04T09:40:28Z | - |
dc.date.issued | 2016-01-01 | - |
dc.identifier.issn | 16 324 | - |
dc.identifier.uri | http://142.54.178.187:9060/xmlui/handle/123456789/1880 | - |
dc.description.abstract | Optical emission spectroscopy is used to investigate the nitrogen-hydrogen with trace rare gas (4% Ar) plasma generated by 50 Hz pulsed DC discharges. The filling pressure varies from 1 mbar to 5 mbar and the current density ranges from 1 mAcenterdotcm−2 to 4 mAcenterdotcm−2. The hydrogen concentration in the mixture plasma varies from 0% to 80%, with the objective of identifying the optimum pressure, current density and hydrogen concentration for active species ([N] and [N2]) generation. It is observed that in an N2-H2 gas mixture, the concentration of N atom density decreases with filling pressure and increases with current density, with other parameters of the discharge kept unchanged. The maximum concentrations of active species were found for 40% H2 in the mixture at 3 mbar pressure and current density of 4 mAcenterdotcm−2. | en_US |
dc.language.iso | en_US | en_US |
dc.publisher | Institute of Physics | en_US |
dc.subject | Natural Science | en_US |
dc.subject | Investigation | en_US |
dc.subject | 50 Hz | en_US |
dc.subject | Nitrogen Plasma | en_US |
dc.subject | Screen Cage | en_US |
dc.subject | Rare Gas | en_US |
dc.subject | Optical Emission | en_US |
dc.subject | Spectroscopy | en_US |
dc.title | Investigation of 50 Hz Pulsed DC Nitrogen Plasma with Active Screen Cage by Trace Rare Gas Optical Emission Spectroscopy | en_US |
dc.type | Article | en_US |
Appears in Collections: | Journals |
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