{"help":"Return the metadata of a dataset (package) and its resources. :param id: the id or name of the dataset :type id: string","success":true,"result":[{"id":"81654b14-f843-4e6c-81c3-cfe3f94e8074","name":"characterisation-volume-and-surface-dielectric-barrier-discharges-n2\u2013o2-mixtures-using","title":"Characterisation of volume and surface dielectric barrier discharges in N2\u2013O2 mixtures using optical emission spectroscopy ","author_email":"kogelheide@aept.rub.de","maintainer":"Research Data Repository","maintainer_email":"achim.vonkeudell@rub.de","license_title":"https:\/\/creativecommons.org\/licenses\/by\/4.0\/","notes":"\u003Cp\u003EA volume and a twin surface dielectric barrier discharge (VDBD and SDBD) are generated in different nitrogen\u2013oxygen mixtures at atmospheric pressure by applying damped sinusoidal voltage waveforms with oscillation periods in the microsecond time scale. Both electrode configurations are located inside vacuum vessels and operated in a controlled atmosphere to exclude the influence of surrounding air. The discharges are characterised with different spatial and temporal resolution by applying absolutely calibrated optical emission spectroscopy in conjunction with numerical simulations and current\u2013voltage measurements. Plasma parameters, namely the electron density and the reduced electric field, and the dissipated power are found to depend strongly on the oxygen content in the working gas mixture. Different spatial and temporal distributions of plasma parameters and dissipated power are explained by surface and residual volume charges for different O2 admixtures due to their effects on the electron recombination rate. Thus, the oxygen admixture is found to strongly influence the breakdown process and plasma conditions of a VDBD and a SDBD.\u003C\/p\u003E\n","url":"https:\/\/rdpcidat.rub.de\/dataset\/characterisation-volume-and-surface-dielectric-barrier-discharges-n2%E2%80%93o2-mixtures-using","state":"Active","log_message":"Edited by kd.","private":true,"revision_timestamp":"Mon, 03\/22\/2021 - 12:34","metadata_created":"Fri, 01\/29\/2021 - 14:29","metadata_modified":"Mon, 03\/22\/2021 - 12:34","creator_user_id":"734724ba-213d-4bf5-b2c9-6f56e5b8a1a9","type":"Dataset","resources":[{"id":"af958218-4486-4c8a-9382-a2d019413365","revision_id":"","url":"https:\/\/rdpcidat.rub.de\/sites\/default\/files\/Paper_N2O2.zip","description":"\u003Cp\u003EOriginPro is neede to access the data.\u003C\/p\u003E\n","format":"zip","state":"Active","revision_timestamp":"Wed, 02\/03\/2021 - 12:41","name":"All figures","mimetype":"application\/zip","size":"12.76 MB","created":"Wed, 02\/03\/2021 - 12:36","resource_group_id":"60dfa3fb-4113-4271-8531-8587fa07dcbe","last_modified":"Date changed  Wed, 02\/03\/2021 - 12:41"}],"tags":[{"id":"de73035c-aa02-4b9b-b53d-ac9ed0e63557","vocabulary_id":"2","name":"collisional-radiative model"},{"id":"620845fb-4747-4abd-ad7a-9d2d08b50d24","vocabulary_id":"2","name":"controlles atmosphere"},{"id":"0aad9071-ba5c-43f2-b2df-cc066152c5f8","vocabulary_id":"2","name":"dielectric barrier discharge"},{"id":"097ab695-fe9a-4a01-83cc-fed3336dc0f8","vocabulary_id":"2","name":"optical emission spectroscopy"},{"id":"277ffb14-496f-40c6-ae13-6772740c321e","vocabulary_id":"2","name":"plasma parameters"}],"groups":[{"description":"\u003Cp\u003EThe group \u0022Allgemeine Elektrotechnik und Plasmatechnik\u0022 at the faculty for engineering and information science.\u003C\/p\u003E\n","id":"60dfa3fb-4113-4271-8531-8587fa07dcbe","image_display_url":"https:\/\/rdpcidat.rub.de\/sites\/default\/files\/AEPT2.png","title":"AEPT","name":"group\/aept"}]}]}