{"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":"ed8fe1fe-8503-417e-bc70-1a60ca81971e","name":"impact-electrode-proximity-streamer-breakdown-and-development-pulsed-dielectric-barrier","title":"Impact of the electrode proximity on the streamer breakdown and development of pulsed dielectric barrier discharges - Dataset","author_email":"jente.wubs@inp-greifswald.de","maintainer":"INPTDAT \u2013 The Data Platform for Plasma Technology","maintainer_email":"wissenschafts-it@inp-greifswald.de","license_title":"https:\/\/creativecommons.org\/licenses\/by\/4.0\/","notes":"\u003Cp\u003EPresented data was obtained from the analysis of the impact of the electrode proximity on the streamer breakdown and development of pulsed-driven dielectric barrier discharges (DBDs) in a singlefilament arrangement in a gas mixture of 0.1 vol% O2 in N2 at 0.6 bar and 1.0 bar. The gap distance was varied from 0.5 mm to 1.5 mm, and the applied voltage was adapted correspondingly to create comparable breakdown conditions in the gap. Fast electrical measurements provided insight into discharge characteristics such as the transferred charge and consumed energy. Results show that the proximity of the cathode has a strong impact on the characteristics of the streamer breakdown.\u003C\/p\u003E\n","url":"https:\/\/www.inptdat.de\/dataset\/impact-electrode-proximity-streamer-breakdown-and-development-pulsed-dielectric-barrier","state":"Active","log_message":"Update to resource Impact of the electrode proximity on the streamer breakdown (Figure 2d)","private":true,"revision_timestamp":"Thu, 02\/17\/2022 - 09:21","metadata_created":"Wed, 02\/16\/2022 - 14:22","metadata_modified":"Thu, 02\/17\/2022 - 09:21","creator_user_id":"0e27023c-5517-4b3f-b96e-c939dc6a74ff","type":"Dataset","resources":[{"id":"9adec475-ba35-4b7a-9ee9-7990877b2f01","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node531_figure_2a.csv","description":"\u003Cp\u003EElectrical characteristics of pulsed DBDs with f_rep = 10 kHz and t_pulse = 1e-6 s in a 1.5 mm gap with 0.1 vol % O_2 in N_2 at p = 1 bar. Overview of the applied voltage and corresponding current for V_pulse = 10 kV.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 02\/16\/2022 - 14:21","name":"Impact of the electrode proximity on the streamer breakdown (Figure 2a)","mimetype":"text\/csv","size":"2.03 MB","created":"Mon, 02\/07\/2022 - 10:58","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 02\/16\/2022 - 14:21"},{"id":"dfcb2a12-9045-4b69-9af2-fcfc9c59d70f","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node531_figure_2b.csv","description":"\u003Cp\u003EElectrical characteristics of pulsed DBDs with f_rep = 10 kHz and t_pulse = 1e-6 s in a 1.5 mm gap with 0.1 vol % O_2 in N_2 at p = 1 bar. Rising slope in detail for V_pulse = 10 kV.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 02\/16\/2022 - 14:21","name":"Impact of the electrode proximity on the streamer breakdown (Figure 2b)","mimetype":"text\/csv","size":"64.37 KB","created":"Mon, 02\/07\/2022 - 11:12","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 02\/16\/2022 - 14:21"},{"id":"3b41656c-3e8e-456c-bba7-5f155b7e5642","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node531_figure_2c.csv","description":"\u003Cp\u003EElectrical characteristics of pulsed DBDs with f_rep = 10 kHz and t_pulse = 1e-6 s in a 1.5 mm gap with 0.1 vol % O_2 in N_2 at p = 1 bar. Discharge current at the rising slope for V_pulse = 10 - 14 kV.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 02\/16\/2022 - 14:21","name":"Impact of the electrode proximity on the streamer breakdown (Figure 2c)","mimetype":"text\/csv","size":"132.55 KB","created":"Mon, 02\/07\/2022 - 11:30","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 02\/16\/2022 - 14:21"},{"id":"b68f26f3-890f-4ef7-95bd-3a50df86810c","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node531_figure_2d.csv","description":"\u003Cp\u003EElectrical characteristics of pulsed DBDs with f_rep = 10 kHz and t_pulse = 1e-6 s in a 1.5 mm gap with 0.1 vol % O_2 in N_2 at p = 1 bar.  Q-V plot providing the capacitances of the arrangement and the consumed electrical energy per pulse.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 02\/16\/2022 - 14:21","name":"Impact of the electrode proximity on the streamer breakdown (Figure 2d)","mimetype":"text\/csv","size":"3.15 MB","created":"Mon, 02\/07\/2022 - 11:39","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 02\/16\/2022 - 14:21"},{"id":"1d43f27e-f7f9-4312-95cb-20da547e5b90","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node531_figure_3a.csv","description":"\u003Cp\u003EElectrical properties of the selected DBDs for different gap distances and pressures. Maximum of the discharge current.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 02\/16\/2022 - 14:21","name":"Impact of the electrode proximity on the streamer breakdown (Figure 3a)","mimetype":"text\/csv","size":"194 bytes","created":"Mon, 02\/07\/2022 - 11:48","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 02\/16\/2022 - 14:21"},{"id":"49d8b5da-18ad-4a1a-b7e4-ffa56619bdb4","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node531_figure_3b.csv","description":"\u003Cp\u003EElectrical properties of the selected DBDs for different gap distances and pressures. Transferred charge per single DBD and consumed electrical energy per HV period.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 02\/16\/2022 - 14:21","name":"Impact of the electrode proximity on the streamer breakdown (Figure 3b)","mimetype":"text\/csv","size":"498 bytes","created":"Mon, 02\/07\/2022 - 11:55","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 02\/16\/2022 - 14:21"},{"id":"226eb3f8-3a9c-4cc4-b599-4f6b6778e3b4","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node531_figure_5a_0.csv","description":"\u003Cp\u003EComparison of the discharge diameter d_DBD at the rising slope for different gap distances at p = 1.0 bar.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 02\/16\/2022 - 14:21","name":"Impact of the electrode proximity on the streamer breakdown (Figure 5a)","mimetype":"text\/csv","size":"41.99 KB","created":"Tue, 02\/08\/2022 - 15:06","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 02\/16\/2022 - 14:21"},{"id":"e30538fa-fef1-4ff7-a6af-7c042607f28f","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node531_figure_5b.csv","description":"\u003Cp\u003EComparison of the discharge diameter d_DBD at the rising slope for different gap distances at p = 0.6 bar.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 02\/16\/2022 - 14:21","name":"Impact of the electrode proximity on the streamer breakdown (Figure 5b)","mimetype":"text\/csv","size":"41.92 KB","created":"Tue, 02\/08\/2022 - 15:12","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 02\/16\/2022 - 14:21"},{"id":"6130377f-2ef4-4c48-a8ea-3f10b8dca794","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node531_figure_7.csv","description":"\u003Cp\u003EContour plots extracted from streak images illustrating the propagation of the cathode-directed streamer at the rising slope for different gap distances at p = 1.0 bar. For a better comparison, the curves were shifted in time to reach the cathode at the same time t = t_0.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 02\/16\/2022 - 14:21","name":"Impact of the electrode proximity on the streamer breakdown (Figure 7)","mimetype":"text\/csv","size":"123.34 KB","created":"Tue, 02\/08\/2022 - 15:20","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 02\/16\/2022 - 14:21"},{"id":"ffb0f93c-1c23-4508-b575-e0a78be8d9c4","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node531_figure_8a.csv","description":"\u003Cp\u003EPropagation velocity of the cathode-directed streamer at the rising slope for different voltage pulse amplitudes in a 1.5 mm gap for p = 1.0 bar.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 02\/16\/2022 - 14:21","name":"Impact of the electrode proximity on the streamer breakdown (Figure 8a)","mimetype":"text\/csv","size":"5.11 KB","created":"Tue, 02\/08\/2022 - 15:25","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 02\/16\/2022 - 14:21"},{"id":"752e258a-2c20-4101-8df4-c6e9eab400f9","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node531_figure_8b.csv","description":"\u003Cp\u003EPropagation velocity of the cathode-directed streamer at the rising slope for different voltage pulse amplitudes in a 1.5 mm gap for p = 0.6 bar\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 02\/16\/2022 - 14:21","name":"Impact of the electrode proximity on the streamer breakdown (Figure 8b)","mimetype":"text\/csv","size":"5.78 KB","created":"Tue, 02\/08\/2022 - 15:27","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 02\/16\/2022 - 14:21"},{"id":"5ee24245-4ebf-4b6f-800a-40ad10b5e7cd","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node531_figure_9a.csv","description":"\u003Cp\u003EComparison of the streamer propagation velocities at the rising slope for different gap distances (velocity as a function of the distance from the anode).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 02\/16\/2022 - 14:21","name":"Impact of the electrode proximity on the streamer breakdown (Figure 9a)","mimetype":"text\/csv","size":"4.57 KB","created":"Tue, 02\/08\/2022 - 15:30","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 02\/16\/2022 - 14:21"},{"id":"d6c43718-25cd-467b-9abd-a7608e65eb20","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node531_figure_9b.csv","description":"\u003Cp\u003EComparison of the streamer propagation velocities at the rising slope for different gap distances and pressures (velocity as a function of the normalised distance z\u2217, where z\u2217 = z\/d_gap).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Wed, 02\/16\/2022 - 14:21","name":"Impact of the electrode proximity on the streamer breakdown (Figure 9b)","mimetype":"text\/csv","size":"9.71 KB","created":"Tue, 02\/08\/2022 - 15:34","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Wed, 02\/16\/2022 - 14:21"}],"tags":[{"id":"4422fa94-b35f-4970-9732-81fb95852746","vocabulary_id":"2","name":"streamer discharge"}],"groups":[{"description":"\u003Cp\u003E\u003Cstrong\u003ELeibniz Institute for Plasma Science and Technology\u003C\/strong\u003E\u003Cbr \/\u003E\nFelix-Hausdorff-Str. 2\u003Cbr \/\u003E\n17489 Greifswald\u003Cbr \/\u003E\nGERMANY\u003C\/p\u003E\n\u003Cp\u003E\u003Ca href=\u0022https:\/\/www.inp-greifswald.de\/en\/\u0022\u003Ehttps:\/\/www.inp-greifswald.de\/en\/\u003C\/a\u003E\u003Cbr \/\u003E\n\u003Cspan class=\u0022spamspan\u0022\u003E\u003Cspan class=\u0022u\u0022\u003Ewelcome\u003C\/span\u003E\u003Cimg class=\u0022spam-span-image\u0022 alt=\u0022at\u0022 width=\u002210\u0022 src=\u0022\/sites\/all\/modules\/spamspan\/image.gif\u0022 \/\u003E\u003Cspan class=\u0022d\u0022\u003Einp-greifswald\u003Cspan class=\u0022t\u0022\u003E [punkt] \u003C\/span\u003Ede\u003C\/span\u003E\u003C\/span\u003E\u003C\/p\u003E\n\u003Cp align=\u0022justify\u0022\u003EThe Leibniz Institute for Plasma Science and Technology (INP) is the largest non-university institute in the field of low temperature plasmas, their basics and technical applications in Europe. The institute carries out research and development from idea to prototype. The topics focus on the needs of the market. At present, plasmas for materials and energy as well as for environment and health are the focus of interest. \u003C\/p\u003E\n","id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","image_display_url":"https:\/\/www.inptdat.de\/sites\/default\/files\/inp.png","title":"INP","name":"group\/inp"}]}]}