{"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":"747f7a1e-861e-4329-a1bb-2695a58b3acb","name":"electrical-characteristics-atmospheric-pressure-dbd-argon-small-admixtures-tms-measured-and","title":"Electrical characteristics of atmospheric-pressure DBD in argon with small admixtures of TMS - measured and calculated data","author_email":"loffhagen@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\u003EA time-dependent, spatially one-dimensional fluid-Poisson model has been applied to analyse the impact of small amounts of tetramethylsilane (TMS) on the discharge characteristics of an atmospheric-pressure dielectric barrier discharge (DBD) in argon. Based on an established argon kinetics, it includes a reaction kinetics for TMS, which has been validated by measurements of the ignition voltage at the frequency f = 86.2 kHz for TMS amounts of up to 200 ppm. It is found that good agreement between measured and calculated ignition voltage can be obtained, when assuming that 25 % of the reactions of TMS with excited argon atoms with a rate coefficient of 3.0\u00d710^{\u221216} m^3\/s lead to the production of electrons due to Penning ionization. The dataset contains measured and calculated data for the ignition voltage and discharge current.\u003C\/p\u003E\n","url":"https:\/\/www.inptdat.de\/dataset\/electrical-characteristics-atmospheric-pressure-dbd-argon-small-admixtures-tms-measured-and","state":"Active","log_message":"Update to resource Electrical characteristics of atmospheric-pressure DBD in argon with small admixtures of TMS - U,I experiment @ 100 ppm","private":true,"revision_timestamp":"Wed, 05\/11\/2022 - 17:32","metadata_created":"Wed, 08\/12\/2020 - 10:05","metadata_modified":"Wed, 05\/11\/2022 - 17:32","creator_user_id":"0e27023c-5517-4b3f-b96e-c939dc6a74ff","type":"Dataset","resources":[{"id":"bbf059dd-636e-4ed5-98a8-720951ff99e0","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node250_Ui-vs-TMS_0.csv","description":"\u003Cp\u003EIgnition voltages U_i obtained by measurements and by modelling using different parameter sets of k_M,Ar\u2217 and \u03b1_PI in dependence on the TMS fraction x. For the measured data the mean values and difference to minimum (Err_min) and maximum (Err_max) values are given.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 08\/17\/2020 - 13:48","name":"Electrical characteristics of atmospheric-pressure DBD in argon with small admixtures of TMS - ignition voltage","mimetype":"text\/csv","size":"580 bytes","created":"Wed, 08\/12\/2020 - 10:05","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 08\/17\/2020 - 13:48"},{"id":"a8058406-b8db-47c1-b49b-1a2a3be01ff5","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node250_10ppm_U-I_mod20.csv","description":"\u003Cp\u003EApplied voltage U_a and calculated current vs. relative time for the 20th period and TMS fraction x = 10 ppm.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 08\/17\/2020 - 12:43","name":"Electrical characteristics of atmospheric-pressure DBD in argon with small admixtures of TMS - U,I model @ 10 ppm, period 20","mimetype":"text\/csv","size":"12.31 KB","created":"Mon, 08\/17\/2020 - 12:43","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 08\/17\/2020 - 12:43"},{"id":"50ddee4b-5515-45ef-8147-5b1da37434f9","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node250_10ppm_U-I_mod688.csv","description":"\u003Cp\u003EApplied voltage U_a and calculated current vs. relative time for the 688th period and TMS fraction x = 10 ppm.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 08\/17\/2020 - 12:45","name":"Electrical characteristics of atmospheric-pressure DBD in argon with small admixtures of TMS - U,I model @ 10 ppm, period 688","mimetype":"text\/csv","size":"12.31 KB","created":"Mon, 08\/17\/2020 - 12:45","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 08\/17\/2020 - 12:45"},{"id":"98098bf4-87a6-4d41-903a-27eafae23f25","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node250_10ppm_U-I_exp.csv","description":"\u003Cp\u003EApplied voltage U_a and measured current vs. relative time for TMS fraction x = 10 ppm. Data obtained by the capacitor method (C_m) and shunt resistor method (R_m) are given.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 08\/17\/2020 - 12:50","name":"Electrical characteristics of atmospheric-pressure DBD in argon with small admixtures of TMS - U,I experiment @ 10 ppm","mimetype":"text\/csv","size":"408 KB","created":"Mon, 08\/17\/2020 - 12:50","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 08\/17\/2020 - 12:50"},{"id":"df240c91-5fdc-4b2e-952c-d923b0c6aff0","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node250_100ppm_U-I_mod20.csv","description":"\u003Cp\u003EApplied voltage U_a and calculated current vs. relative time for the 20th period and TMS fraction x = 100 ppm.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 08\/17\/2020 - 12:52","name":"Electrical characteristics of atmospheric-pressure DBD in argon with small admixtures of TMS - U,I model @ 100 ppm, period 20","mimetype":"text\/csv","size":"12.31 KB","created":"Mon, 08\/17\/2020 - 12:52","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 08\/17\/2020 - 12:52"},{"id":"4e5f8c75-13a3-4c31-a8d5-9672622345a8","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node250_100ppm_U-I_mod688.csv","description":"\u003Cp\u003EApplied voltage U_a and calculated current vs. relative time for the 688th period and TMS fraction x = 100 ppm.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Mon, 08\/17\/2020 - 12:55","name":"Electrical characteristics of atmospheric-pressure DBD in argon with small admixtures of TMS - U,I model @ 100 ppm, period 688","mimetype":"text\/csv","size":"12.31 KB","created":"Mon, 08\/17\/2020 - 12:53","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Mon, 08\/17\/2020 - 12:55"},{"id":"ecaa7507-39c3-46b8-8cde-99f41ba8bb5b","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node250_100ppm_U-I_exp.csv","description":"\u003Cp\u003EApplied voltage U_a and measured current vs. relative time for TMS fraction x = 100 ppm. Data obtained by the capacitor method (C_m) and shunt resistor method (R_m) are given.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Fri, 06\/11\/2021 - 12:36","name":"Electrical characteristics of atmospheric-pressure DBD in argon with small admixtures of TMS - U,I experiment @ 100 ppm","mimetype":"text\/csv","size":"408 KB","created":"Mon, 08\/17\/2020 - 12:56","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Fri, 06\/11\/2021 - 12:36"}],"tags":[{"id":"0f896bf1-4b70-4087-90c3-86d89112b1aa","vocabulary_id":"2","name":"plasma modelling\/simulation"},{"id":"8dde877f-9b50-4dd2-a90d-8f69ad86a950","vocabulary_id":"2","name":"DBD"},{"id":"b4385324-8681-4532-80ab-b6fdd2da79ee","vocabulary_id":"2","name":"TMS"}],"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"},{"description":"\u003Cp\u003ETechnische Universit\u00e4t Braunschweig\u003Cbr \/\u003E\n\u003Cstrong\u003EInstitute for Surface Technology\u003C\/strong\u003E\u003Cbr \/\u003E\nBienroder Weg 54E\u003Cbr \/\u003E\nD 38108 Braunschweig\u003Cbr \/\u003E\nGERMANY\u003C\/p\u003E\n\u003Cp\u003E\u003Ca href=\u0022https:\/\/www.tu-braunschweig.de\/en\/iot\u0022\u003EHomepage\u003C\/a\u003E\u003C\/p\u003E\n\u003Cp align=\u0022justify\u0022\u003EThe Institute of Surface Technology is engaged in research and education in the field of production, characterization and application of thin films and surface modification. Besides the topics from mechanical and automotive engineering, the institute is active in all fields where function-optimized surfaces are used or required.\u003C\/p\u003E\n","id":"3aef3ef3-f440-4e87-96f0-a58bf6c0669a","image_display_url":"https:\/\/www.inptdat.de\/sites\/default\/files\/Logo_IOT_lang_englisch.png","title":"IOT","name":"group\/iot"}]}]}