{"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":"79d57267-7e4a-4734-9b5a-7969617649b8","name":"modelling-microarcs-copper-metal-vapour-dominated-air","title":"Modelling of microarcs in copper metal vapour dominated air","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 dominated by copper metal vapour. The plasma is generated between copper electrodes.  The model resembles the microarcs that occur at low-voltage and low-current conditions in switching devices during a contact separation.  Data concerning the plasma parameters, including electric potential, temperatures of electron and heavy particles, number densities of charged and neutral species are provided as tables.\u003C\/p\u003E\n","url":"https:\/\/www.inptdat.de\/dataset\/modelling-microarcs-copper-metal-vapour-dominated-air","state":"Active","log_message":"Update to resource Modelling of microarcs in copper metal vapour dominated air - Fig6b","private":true,"revision_timestamp":"Tue, 09\/16\/2025 - 08:13","metadata_created":"Mon, 10\/07\/2024 - 14:14","metadata_modified":"Tue, 09\/16\/2025 - 08:13","creator_user_id":"d52069c6-138a-4a56-9553-eddea8f72c53","type":"Dataset","resources":[{"id":"6dd13aad-aa64-4e55-9424-4b156286bd3c","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node871_Fig1.csv","description":"\u003Cp\u003EThe rate coefficients for direct ionization (Kid), step-wise ionization (Kis), and the total ionization (Ki) of Cu atoms as a function of the electron temperature.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 09\/16\/2025 - 08:13","name":"Modelling of microarcs in copper metal vapour dominated air - Fig1","mimetype":"text\/csv","size":"524.75 KB","created":"Thu, 12\/05\/2024 - 14:56","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 09\/16\/2025 - 08:13"},{"id":"a81f259b-5428-442c-b7c1-e3dc8abafc66","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node871_Fig2a.csv","description":"\u003Cp\u003EDistribution of the electric potential in the plasma region for a gap length of 30 \u00b5m (Rdis= 155  \u00b5m) and FEF-values of 250  and 300.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 09\/16\/2025 - 08:13","name":"Modelling of microarcs in copper metal vapour dominated air - Fig2a","mimetype":"text\/csv","size":"160.98 KB","created":"Thu, 12\/05\/2024 - 15:04","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 09\/16\/2025 - 08:13"},{"id":"9b1a3fc4-2e0d-4331-9b1a-25aaa599b5f2","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node871_Fig2b.csv","description":"\u003Cp\u003EDistribution of the electric potential in the plasma region for a gap lengths of 300 \u00b5m (Rdis= 250  \u00b5m) , and FEF-values of 250  and 300.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 09\/16\/2025 - 08:13","name":"Modelling of microarcs in copper metal vapour dominated air - Fig2b","mimetype":"text\/csv","size":"161.87 KB","created":"Thu, 12\/05\/2024 - 15:10","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 09\/16\/2025 - 08:13"},{"id":"31eb06d1-df6f-47be-a65a-0b4243704938","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node871_Fig3.csv","description":"\u003Cp\u003EDistribution of the electric potential in the plasma region for gap lengths of 300 \u00b5m and discharge radii Rdis of 200 \u00b5m, 250 \u00b5m, and 300 \u00b5m. 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