{"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":"7fb50ba4-38ca-471d-b2d4-7b6e17ee9c04","name":"reversal-electric-field-and-anode-fall-dc-arcs-air-during-contact-opening","title":"Reversal of the electric field and the anode fall in DC arcs in air during contact opening","author":"DO NOT USE","author_email":"baeva@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\u003EThe dataset contains results of a unified one-dimensional model of an arc plasma in air, between copper electrodes, that includes the change of the gap distance. The occurance of multiple reversals of the electric field and the anode voltage drop is observed. The evolution of the spatial distribution of the electron and heavy particle temperatures with the gap distance and the opening speed is also studied. The model quantitatively predicts a number of plasma properties under conditions that are relevant to the contact separation in low-voltage switching devices.\u003C\/p\u003E\n","url":"https:\/\/www.inptdat.de\/dataset\/reversal-electric-field-and-anode-fall-dc-arcs-air-during-contact-opening","state":"Active","log_message":"Update to resource Reversal of the electric field and the anode fall in DC arcs - Fig4b","private":true,"revision_timestamp":"Mon, 12\/09\/2024 - 16:58","metadata_created":"Fri, 05\/24\/2024 - 13:14","metadata_modified":"Mon, 12\/09\/2024 - 16:58","creator_user_id":"0e27023c-5517-4b3f-b96e-c939dc6a74ff","type":"Dataset","resources":[{"id":"c7de3a88-bf6d-4e69-845e-e8d41200d47d","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node830_Fig1_0.csv","description":"\u003Cp\u003EThe graph presents the curent density (in units of A\/m^2) caused by thermo-field emission as a function of the surface electric field (in units of V\/m) for a number of temperatures on the cathode surface (T in units of K).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Fri, 06\/28\/2024 - 10:52","name":"Reversal of the electric field and the anode fall in DC arcs - Fig1","mimetype":"text\/csv","size":"3.22 KB","created":"Tue, 06\/04\/2024 - 15:00","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Fri, 06\/28\/2024 - 10:52"},{"id":"50211373-af05-4113-ab6a-2724ec7398f8","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node830_Fig2_1.csv","description":"\u003Cp\u003EThe distribution of the electric potential in the inter-electrode gap for an opening times of 1 ms. The cathode is at position 0 mm, that of the anode varies from 0.03 mm up to 1 mm.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Fri, 06\/28\/2024 - 10:52","name":"Reversal of the electric field and the anode fall in DC arcs - Fig2-1","mimetype":"text\/csv","size":"405.75 KB","created":"Wed, 06\/05\/2024 - 09:05","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Fri, 06\/28\/2024 - 10:52"},{"id":"ceb352bd-b1ec-46b1-a7da-e0d3e6b69d8d","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node830_Fig2_2.csv","description":"\u003Cp\u003EThe distribution of the electric potential in the inter-electrode gap for opening times of 1 s. The cathode is at position 0 mm, that of the anode varies from 0.03 mm up to 1 mm.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Fri, 06\/28\/2024 - 10:52","name":"Reversal of the electric field and the anode fall in DC arcs - Fig2-2","mimetype":"text\/csv","size":"405.67 KB","created":"Wed, 06\/05\/2024 - 09:06","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Fri, 06\/28\/2024 - 10:52"},{"id":"eaa57c5f-5f7a-4b5b-b5ea-d7e56b274d24","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node830_Fig2_3.csv","description":"\u003Cp\u003EThe distribution of the electric potential in the inter-electrode gap for step-wise contact opening. The cathode is at position 0 mm, that of the anode varies from 0.03 mm up to 1 mm.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Fri, 06\/28\/2024 - 10:52","name":"Reversal of the electric field and the anode fall in DC arcs - Fig2-3","mimetype":"text\/csv","size":"1.28 MB","created":"Wed, 06\/05\/2024 - 09:08","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Fri, 06\/28\/2024 - 10:52"},{"id":"49c51d81-4f1a-4f76-85f1-4fc5da57bab9","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node830_Fig3.csv","description":"\u003Cp\u003EThe distribution of the electric field magnitude in the inter-electrode gap for an opening time of 1 ms. The anode is at positions from 0.2 mm up to 1 mm.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Fri, 06\/28\/2024 - 10:52","name":"Reversal of the electric field and the anode fall in DC arcs - Fig3","mimetype":"text\/csv","size":"184.32 KB","created":"Wed, 06\/05\/2024 - 09:09","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Fri, 06\/28\/2024 - 10:52"},{"id":"80e0e40c-b644-4a89-8741-8eac42c6b0a2","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node830_Fig4a.csv","description":"\u003Cp\u003EThe distribution of the electron temperature in the interelectrode gap for various gap lengths..\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Fri, 06\/28\/2024 - 10:52","name":"Reversal of the electric field and the anode fall in DC arcs - Fig4a","mimetype":"text\/csv","size":"184.57 KB","created":"Wed, 06\/05\/2024 - 09:10","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Fri, 06\/28\/2024 - 10:52"},{"id":"be9ece4e-e93f-49cf-9d80-d73419f54706","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node830_Fig4b.csv","description":"\u003Cp\u003EThe distribution of the gas temperature in the interelectrode gap for various gap lengths.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Fri, 06\/28\/2024 - 10:52","name":"Reversal of the electric field and the anode fall in DC arcs - Fig4b","mimetype":"text\/csv","size":"185.25 KB","created":"Wed, 06\/05\/2024 - 09:11","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Fri, 06\/28\/2024 - 10:52"},{"id":"3047da0e-114e-453a-8d4c-ced66b21a5f5","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node830_Fig5.csv","description":"\u003Cp\u003EThe total ionization rate in the interelectrode gap for various gap lengths..\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Fri, 06\/28\/2024 - 10:52","name":"Reversal of the electric field and the anode fall in DC arcs - Fig5","mimetype":"text\/csv","size":"185.16 KB","created":"Wed, 06\/05\/2024 - 09:12","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Fri, 06\/28\/2024 - 10:52"}],"tags":[{"id":"7743f09a-31cb-491d-b605-c91880f851a4","vocabulary_id":"2","name":"unified description"},{"id":"4708b154-f9b5-48cf-b9c5-a1e4e90f44db","vocabulary_id":"2","name":"microarc"},{"id":"4e68bed6-e2f8-4570-bcb5-80a8fc6b8f1f","vocabulary_id":"2","name":"copper electrodes"},{"id":"a7fdbcbd-fbf1-4976-8e66-73a48d92a84c","vocabulary_id":"2","name":"anode fall"},{"id":"92a0c847-5028-4af8-a692-80aa993b1add","vocabulary_id":"2","name":"field reversal"}],"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"}]}]}