{"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":"7a581f22-499c-4050-b2bb-09dab8f881bd","name":"effect-spatially-fluctuating-heating-particles-plasma-spray-process-dataset","title":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Dataset","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 work is concerned with the effect of a spatially fluctuating heating of Al_2O_3 particles with diameters of 5\u2013120 \u03bcm during a plasma spray process. A plasma jet is generated in a mixture of Ar (40 NLPM) and H_2 (14 NLPM) and in pure Ar at an electric current of 600 A. The tracing of the injected particles in the plume region of the plasma jets is considered in the framework of a three-dimensional model taking into account a turbulent fluid flow. It is shown that the heat source for the injected particles exhibits a well pronounced spatially fluctuating structure due to the enhancement of the thermal conductivity resulting from dissociation and ionization of the molecular gas in the temperature range of 2500\u20134000 K and 13000\u201314000 K, respectively. During their travel towards the substrate, the particles are therefore repeatedly heated in the gas mixture in contrast to the case of pure argon. Particles injected in the gas mixture reach the substrate with a higher average temperature and velocity.\u003C\/p\u003E\n","url":"https:\/\/www.inptdat.de\/dataset\/effect-spatially-fluctuating-heating-particles-plasma-spray-process-dataset","state":"Active","log_message":"Update to resource Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig9c","private":true,"revision_timestamp":"Tue, 09\/16\/2025 - 08:13","metadata_created":"Fri, 05\/13\/2022 - 14:07","metadata_modified":"Tue, 09\/16\/2025 - 08:13","creator_user_id":"d52069c6-138a-4a56-9553-eddea8f72c53","type":"Dataset","resources":[{"id":"fc3c40e1-733f-4a0b-a5c3-184d49e009e2","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig2a_0.csv","description":"\u003Cp\u003EData provide two-dimensional temperature distribution in the central plane (X-Z) of the jet plume operating in pure Ar with a flow rate of 40 NLPM. Electric current in the torch is 600 A. The first column contains the axial position z in units of mm, the second one contains the radial position in units of mm, and the third one gives the temperature T in units of K.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig2a","mimetype":"text\/csv","size":"50.98 KB","created":"Tue, 10\/04\/2022 - 10:14","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"ae56292b-ae19-4b64-8284-21fc09a4c7fa","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig2b.csv","description":"\u003Cp\u003EData provide two-dimensional temperature distribution in the central plane (X-Z) of the jet plume operating in a mixture Ar (40 NLPM) - H_2 (14 NLPM). Electric current in the torch is 600 A. The first column contains the axial position z in units of mm, the second one contains the radial position in units of mm, and the third one gives the temperature T in units of K.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig2b","mimetype":"text\/csv","size":"51.11 KB","created":"Tue, 10\/04\/2022 - 10:24","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"93b68fd7-99b4-4d26-8e60-e6228555836e","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig3a.csv","description":"\u003Cp\u003EResults for the pure Ar (40 NLPM) and mixture Ar(40 NLPM) - H_2(14 NLPM), arc current 600 A. The table gives the values of temperature T (K) along the axis of symmetry as a function of the axial distance z (mm) (first column).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig3a","mimetype":"text\/csv","size":"2.87 KB","created":"Tue, 10\/04\/2022 - 11:00","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"3ed9f616-f9f2-41a3-aec7-53ebe7ca8d11","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig3b.csv","description":"\u003Cp\u003EResults for the pure Ar (40 NLPM) and mixture Ar (40 NLPM) - H_2 (14 NLPM), arc current 600 A . The table gives the axial velocity u (m\/s) as a function of the axial distance z (mm) (first column).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig3b","mimetype":"text\/csv","size":"2.93 KB","created":"Tue, 10\/04\/2022 - 11:15","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"b44d159d-bc74-4315-be58-3cc4f76e707d","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig4a.csv","description":"\u003Cp\u003EData provide two-dimensional distribution of the thermal conductivity \u03bb in the central plane (X-Z) of the jet plume operating in pure Ar with a flow rate of 40 NLPM. Electric current in the torch is 600 A. The first column contains the axial position z in units of mm, the second one contains the radial position in units of mm, and the third one gives the thermal conductivity \u03bb in units of W\/m\/K.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig4a","mimetype":"text\/csv","size":"55.18 KB","created":"Tue, 10\/04\/2022 - 11:21","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"6a0585a4-e887-497a-b940-9dea3e8c799b","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig4b.csv","description":"\u003Cp\u003EData provide two-dimensional distribution of the thermal conductivity \u03bb in the central plane (X-Z) of the jet plume operating in a mixture Ar (40 NLPM) - H_2 (14 NLPM). Electric current in the torch is 600 A. The first column contains the axial position z in units of mm, the second one contains the radial position in units of mm, and the third one gives the thermal conductivity \u03bb in units of W\/m\/K.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig4b","mimetype":"text\/csv","size":"117.88 KB","created":"Tue, 10\/04\/2022 - 11:26","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"980dabe1-2c9a-4e08-8e84-db9ac5c6f67a","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig5a.csv","description":"\u003Cp\u003EData provide two-dimensional distribution of the effective thermal conductivity \u03bb+\u03bb_T in the central plane (X-Z) of the jet plume operating in pure Ar with a flow rate of 40 NLPM. Electric current in the torch is 600 A. The first column contains the axial position z in units of mm, the second one contains the radial position in units of mm, and the third one gives the effective thermal conductivity \u03bb+\u03bb_T in units of W\/m\/K.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig5a","mimetype":"text\/csv","size":"53.4 KB","created":"Tue, 10\/04\/2022 - 11:33","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"27f62fe0-1a8a-46fc-8a67-36a92dc6d3cf","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig5b.csv","description":"\u003Cp\u003EData provide two-dimensional distribution of the effective thermal conductivity \u03bb+\u03bb_T in the central plane (X-Z) of the jet plume operating in a mixture Ar (40 NLPM) - H_2 (14 NLPM). Electric current in the torch is 600 A. The first column contains the axial position z in units of mm, the second one contains the radial position in units of mm, and the third one gives the effective thermal conductivity \u03bb+\u03bb_T in units of W\/m\/K.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig5b","mimetype":"text\/csv","size":"53.17 KB","created":"Tue, 10\/04\/2022 - 11:39","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"5ab237f5-59ee-4e4e-8ed2-e2610d34ea2a","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig6a.csv","description":"\u003Cp\u003EData provide the temperature of the plasma jet T related to the selected particles P658 and P678 injected in pure argon and a mixture Ar (40 NLPM) - H2 (14 NLPM) as a function of the axial position z (mm) crossed by the particles.\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumns 1 and 2: z and T for line 1 (P658 in Ar-H_2),\u003Cbr \/\u003E\ncolumns 3 and 4: z and T for line 2 (P658 in Ar),\u003Cbr \/\u003E\ncolumns 5 and 6: z and T for line 3 (P678 in Ar-H_2),\u003Cbr \/\u003E\ncolumns 7 and 8: z and T for line 4 (P678 in Ar).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig6a","mimetype":"text\/csv","size":"33.53 KB","created":"Tue, 10\/04\/2022 - 11:48","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"3b2dad0c-3743-44c3-8a9d-59abc8c1d667","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig6b.csv","description":"\u003Cp\u003EData provide the heat source  Qconv (W) related to the selected particles P658 and P678 injected in pure argon and a mixture Ar (40 NLPM) - H2 (14 NLPM) as a function of the axial position z (mm) crossed by the particles.\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumns 1 and 2: z and Qconv for line 1 (P658 in Ar-H_2),\u003Cbr \/\u003E\ncolumns 3 and 4: z and Qconv for line 2 (P658 in Ar),\u003Cbr \/\u003E\ncolumns 5 and 6: z and Qconv for line 3 (P678 in Ar-H_2),\u003Cbr \/\u003E\ncolumns 7 and 8: z and Qconv for line 4 (P678 in Ar).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig6b","mimetype":"text\/csv","size":"41.48 KB","created":"Tue, 10\/04\/2022 - 11:55","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"0e0efba3-d434-4e99-befb-af3617fff2ca","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig6c_0.csv","description":"\u003Cp\u003EData provide the radiative loss  -Qr (W) related to the selected particles P658 and P678 injected in pure argon and a mixture Ar (40 NLPM) - H2 (14 NLPM) as a function of the axial position z (mm) crossed by the particles.\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumns 1 and 2: z and -Qr for line 1 (P658 in Ar-H_2),\u003Cbr \/\u003E\ncolumns 3 and 4: z and -Qr for line 2 (P658 in Ar),\u003Cbr \/\u003E\ncolumns 5 and 6: z and -Qr for line 3 (P678 in Ar-H_2),\u003Cbr \/\u003E\ncolumns 7 and 8: z and -Qr for line 4 (P678 in Ar).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig6c","mimetype":"text\/csv","size":"44.52 KB","created":"Tue, 10\/04\/2022 - 12:06","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"03cbcfda-3517-4c8b-9795-2a5dc9b18f54","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig6d.csv","description":"\u003Cp\u003EData provide the particle temperature T_p (K)   related to the selected particles P658 and P678 injected in pure argon and a mixture Ar (40 NLPM) - H2 (14 NLPM) as a function of the axial position z (mm) crossed by the particles. A marker on the temperature axis stands for the melting temperature T_m (2327 K).\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumns 1 and 2: z and Tp for line 1 (P658 in Ar-H_2),\u003Cbr \/\u003E\ncolumns 3 and 4: z and Tp for line 2 (P658 in Ar),\u003Cbr \/\u003E\ncolumns 5 and 6: z and Tp for line 3 (P678 in Ar-H_2),\u003Cbr \/\u003E\ncolumns 7 and 8: z and Tp for line 4 (P678 in Ar).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig6d","mimetype":"text\/csv","size":"33.48 KB","created":"Tue, 10\/04\/2022 - 12:11","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"c7ed098d-1378-4530-9c32-432c912abdbe","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig6e.csv","description":"\u003Cp\u003EData provide the modulus of particle velocity v (m\/s)  related to the selected particles P658 and P678 injected in pure argon and a mixture Ar (40 NLPM) - H_2 (14 NLPM) as a function of the axial position z (mm) crossed by the particles.\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumns 1 and 2: z and v for line 1 (P658 in Ar-H_2),\u003Cbr \/\u003E\ncolumns 3 and 4: z and v for line 2 (P658 in Ar),\u003Cbr \/\u003E\ncolumns 5 and 6: z and v for line 3 (P678 in Ar-H_2),\u003Cbr \/\u003E\ncolumns 7 and 8: z and v for line 4 (P678 in Ar).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig6e","mimetype":"text\/csv","size":"33.5 KB","created":"Tue, 10\/04\/2022 - 12:17","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"514687e9-70e5-4ae2-ae9a-6b451584e663","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig8.csv","description":"\u003Cp\u003EThe particle temperature Tp and velocity v obtained by monitoring with the Tecnar Accuraspray-g3c system.  The measurement points are collected during an operation time of 40 hours.\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: time in units of hours,\u003Cbr \/\u003E\ncolumn 2: velocity in units of m\/s,\u003Cbr \/\u003E\ncolumn 3: standard deviation of velocity in units of m\/s,\u003Cbr \/\u003E\ncolumn 4: particle temperature in units of K,\u003Cbr \/\u003E\ncolumn 5: standard deviation of particle temperature in units of m\/s.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig8","mimetype":"text\/csv","size":"557 bytes","created":"Tue, 10\/04\/2022 - 12:27","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"42439234-ab19-480b-bf5e-4561976913c9","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig9a.csv","description":"\u003Cp\u003EData show the particle temperature on the X-Y substrate plane, which is placed at axial position z = 12 cm for particles injected in a mixture Ar (40 NLPM) - H_2 (14 NLPM).\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: horizontal position y in units of mm,\u003Cbr \/\u003E\ncolumn 2: vertical position x in units of mm,\u003Cbr \/\u003E\ncolumn 3: particle temperature in units of K.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig9a","mimetype":"text\/csv","size":"54.83 KB","created":"Tue, 10\/04\/2022 - 12:34","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"960a2036-7eed-4e14-8ac1-da00a20951a6","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig9b.csv","description":"\u003Cp\u003EData represent particle velocity on the X-Y substrate plane, which is placed at axial position z = 12 cm for particles injected in the Ar-H_2 mixture.\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: horizontal position y in units of mm,\u003Cbr \/\u003E\ncolumn 2: vertical position x in units of mm,\u003Cbr \/\u003E\ncolumn 3: particle velocity in units of m\/s.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig9b","mimetype":"text\/csv","size":"55 KB","created":"Tue, 10\/04\/2022 - 12:38","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"ad05a520-aae2-491d-93c1-c817fd1ca5e3","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig9c.csv","description":"\u003Cp\u003EData represent particle temperature on the X-Y substrate plane, which is placed at axial position z = 12 cm for particles injected in pure Ar.\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: horizontal position y in units of mm,\u003Cbr \/\u003E\ncolumn 2: vertical position x in units of mm,\u003Cbr \/\u003E\ncolumn 3: particle temperature in units of K.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig9c","mimetype":"text\/csv","size":"50.59 KB","created":"Tue, 10\/04\/2022 - 12:39","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"aac3a6af-c2ad-48a5-a63b-ab02e85ca0a7","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig9d.csv","description":"\u003Cp\u003EData represent particle velocity on the X-Y substrate plane, which is placed at axial position z = 12 cm for particles injected in pure Ar.\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: horizontal position y in units of mm,\u003Cbr \/\u003E\ncolumn 2: vertical position x in units of mm,\u003Cbr \/\u003E\ncolumn 3: particle velocity in units of m\/s.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig9d","mimetype":"text\/csv","size":"50.76 KB","created":"Tue, 10\/04\/2022 - 12:46","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"b46b2cfa-2e68-4927-b514-a3776d85095f","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig10a.csv","description":"\u003Cp\u003EData present particle size d_p on the X-Y substrate plane, which is placed at axial position z = 12 cm for particles injected in the Ar-H_2 mixture.\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: horizontal position y in units of mm,\u003Cbr \/\u003E\ncolumn 2: vertical position x in units of mm,\u003Cbr \/\u003E\ncolumn 3: particle size d_p in units of \u00b5m.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig10a","mimetype":"text\/csv","size":"55.01 KB","created":"Tue, 10\/04\/2022 - 14:40","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"aeb9fd4f-4255-432e-8858-ea369aaca891","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig10b.csv","description":"\u003Cp\u003EData present computed K-Sommerfield number on the X-Y substrate plane, which is placed at axial position z = 12 cm for particles injected in the Ar-H_2 mixture.\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: horizontal position y in units of mm,\u003Cbr \/\u003E\ncolumn 2: vertical position x in units of mm,\u003Cbr \/\u003E\ncolumn 3: K-Sommerfield number in units of 1.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig10b","mimetype":"text\/csv","size":"54.98 KB","created":"Tue, 10\/04\/2022 - 14:49","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"aeccb429-c380-445e-98da-26fe3c758143","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig10c_0.csv","description":"\u003Cp\u003EData present particle size d_p on the X-Y substrate plane, which is placed at axial position z = 12 cm for particles injected in the Ar-H_2 mixture.\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: horizontal position y in units of mm,\u003Cbr \/\u003E\ncolumn 2: vertical position x in units of mm,\u003Cbr \/\u003E\ncolumn 3: particle size dp in units of \u00b5m.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig10c","mimetype":"text\/csv","size":"50.8 KB","created":"Tue, 10\/04\/2022 - 14:55","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"9f9801f9-7f87-4414-b1a3-daf5c183c34b","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig10d.csv","description":"\u003Cp\u003EData represent computed K-Sommerfield number on the X-Ysubstrate plane, which is placed at axial position z=12 cm for particles injected in pure Ar.\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: horizontal position y in units of mm,\u003Cbr \/\u003E\ncolumn 2: vertical position x in units of mm,\u003Cbr \/\u003E\ncolumn 3: K-Sommerfield number in units of 1.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig10d","mimetype":"text\/csv","size":"50.78 KB","created":"Tue, 10\/04\/2022 - 15:01","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"224a4c3d-3c51-49d4-b22f-920847797eee","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig11a_0.csv","description":"\u003Cp\u003EData provide the computed particle trajectory given by the radial and the axial positions of various materials along the distance.\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 2: computed radial position of the particle made of Al_2O_3,\u003Cbr \/\u003E\ncolumn 3: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 4: computed radial position of the particle made of iron,\u003Cbr \/\u003E\ncolumn 5: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 6: computed radial position of the particle made of ZrO_2 (dense),\u003Cbr \/\u003E\ncolumn 7: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 8: computed radial position of the particle made of ZrO_2 (porous),\u003Cbr \/\u003E\ncolumn 9: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 10: radial position of the particle made of Al_2O_3 from literature,\u003Cbr \/\u003E\ncolumn 11: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 12: radial position of the particle made of iron from literature,\u003Cbr \/\u003E\ncolumn 13: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 14: radial position of the particle made of ZrO_2 (dense) from literature,\u003Cbr \/\u003E\ncolumn 15: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 16: radial position of the particle made of ZrO_2 (porous) from literature.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig11a","mimetype":"text\/csv","size":"59.04 KB","created":"Tue, 10\/04\/2022 - 15:26","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"e9626ce8-3f42-4d9f-a1e8-f9d637f71e48","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig11b_0.csv","description":"\u003Cp\u003EData provide the computed particle velocity of particles of various materials along the distance z in comparison with published data in the work by Djebali et al. [7].\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 2: computed velocity of the particle made of Al_2O_3,\u003Cbr \/\u003E\ncolumn 3: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 4: computed velocity of the particle made of iron,\u003Cbr \/\u003E\ncolumn 5: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 6: computed velocity of the particle made of ZrO_2 (dense),\u003Cbr \/\u003E\ncolumn 7: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 8: computed velocity of the particle made of ZrO_2 (porous),\u003Cbr \/\u003E\ncolumn 9: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 10: velocity of the particle made of Al_2O_3 from literature,\u003Cbr \/\u003E\ncolumn 11: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 12: velocity of the particle made of iron from literature,\u003Cbr \/\u003E\ncolumn 13: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 14: velocity of the particle made of ZrO_2 (dense) from literature,\u003Cbr \/\u003E\ncolumn 15: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 16: velocity of the particle made of ZrO_2 (porous) from literature.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig11b","mimetype":"text\/csv","size":"58.45 KB","created":"Tue, 10\/04\/2022 - 15:40","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"e63e7d04-aaaa-4701-a83f-c8251f567579","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig11c_0.csv","description":"\u003Cp\u003EData provide the computed particle temperature of various materials along the distance z in comparison with published data in the work by Djebali et al. [7].\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 2: computed particle temperature of the particle made of Al_2O_3,\u003Cbr \/\u003E\ncolumn 3: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 4: computed particle temperature of the particle made of iron,\u003Cbr \/\u003E\ncolumn 5: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 6: computed particle temperature of the particle made of ZrO_2(dense),\u003Cbr \/\u003E\ncolumn 7: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 8: computed particle temperature of the particle made of ZrO_2(porous),\u003Cbr \/\u003E\ncolumn 9: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 10: particle temperature of the particle made of Al_2O_3 from literature,\u003Cbr \/\u003E\ncolumn 11: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 12: particle temperature of the particle made of iron from literature,\u003Cbr \/\u003E\ncolumn 13: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 14: particle temperature of the particle made of ZrO_2(dense) from literature,\u003Cbr \/\u003E\ncolumn 15: axial position measured by the distance from the torch exit z (m),\u003Cbr \/\u003E\ncolumn 16: particle temperature of the particle made of ZrO_2(porous) from literature.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig11c","mimetype":"text\/csv","size":"56.81 KB","created":"Tue, 10\/04\/2022 - 16:11","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"badef020-2b49-439f-a248-fd1c746c3278","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig12.csv","description":"\u003Cp\u003EData provide particle size distribution applied in the model of particle tracing. The particle size distribution is measured based on the static light scattering (SLS) technique combined with a Mie scattering model. The SLS experiment was performed employing the Mastersizer 2000 device (Ref. [63] in the paper).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig12","mimetype":"text\/csv","size":"1.44 KB","created":"Tue, 10\/04\/2022 - 16:22","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"75b1a101-307e-4258-967a-c23feb2595fb","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig13a.csv","description":"\u003Cp\u003EData present a comparison of the calculated plasma jet temperature along the jet axis with the results from other models and experiments.\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 2: computed plasma temperature (K) in the present work,\u003Cbr \/\u003E\ncolumn 3: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 4: computed plasma temperature (K) by Djebali et al. (2016),\u003Cbr \/\u003E\ncolumn 5: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 6: measured plasma temperature (K) by Pfender et al.,\u003Cbr \/\u003E\ncolumn 7: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 8: computed plasma temperature (K) by Pfender et al.,\u003Cbr \/\u003E\ncolumn 9: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 10: computed plasma temperature (K) by Jets\u0026amp;Podres,\u003Cbr \/\u003E\ncolumn 11: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 12: computed plasma temperature (K) by Zhang et al.,\u003Cbr \/\u003E\ncolumn 13: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 14: computed plasma temperature (K) by Sun et al.,\u003Cbr \/\u003E\ncolumn 15: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 16: computed plasma temperature (K) by Djebali et al. (2012).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig13a","mimetype":"text\/csv","size":"7.34 KB","created":"Tue, 10\/04\/2022 - 16:37","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"b889142f-939e-4c69-94cf-1bbd91d6db83","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig13b.csv","description":"\u003Cp\u003EData present a comparison of the calculated plasma jet velocity along the jet axis with the results from other models and experiments.\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 2: computed plasma temperature (K) in the present work,\u003Cbr \/\u003E\ncolumn 3: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 4: computed plasma temperature (K) by Djebali et al. (2016),\u003Cbr \/\u003E\ncolumn 5: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 6: measured plasma temperature (K) by Pfender et al.,\u003Cbr \/\u003E\ncolumn 7: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 8: computed plasma temperature (K) by Pfender et al.,\u003Cbr \/\u003E\ncolumn 9: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 10: computed plasma temperature (K) by Jets\u0026amp;Podres,\u003Cbr \/\u003E\ncolumn 11: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 12: computed plasma temperature (K) by Zhang et al.,\u003Cbr \/\u003E\ncolumn 13: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 14: computed plasma temperature (K) by Sun et al.,\u003Cbr \/\u003E\ncolumn 15: axial distance z (mm),\u003Cbr \/\u003E\ncolumn 16: computed plasma temperature (K) by Djebali et al. (2012),\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig13b","mimetype":"text\/csv","size":"7.09 KB","created":"Tue, 10\/04\/2022 - 16:40","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"5a3a0ca2-7b4b-43aa-87f1-887de77756a2","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig14a_0.csv","description":"\u003Cp\u003EData present a comparison of the computed thermal conductivity against published data (Murphy et al.)\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: Plasma temperature (K),\u003Cbr \/\u003E\ncolumn 2: Thermal conductivity (W\/m\/K) for a mixture Ar:H_2=1:1,\u003Cbr \/\u003E\ncolumn 3: Thermal conductivity (W\/m\/K) for a mixture Ar:H_2=1:3 ,\u003Cbr \/\u003E\ncolumn 4: Thermal conductivity (W\/m\/K) for a mixture Ar:H_2=3:1,\u003Cbr \/\u003E\ncolumn 5: Thermal conductivity (W\/m\/K) for pure Ar,\u003Cbr \/\u003E\ncolumn 6: Thermal conductivity (W\/m\/K) for pure H_2,\u003Cbr \/\u003E\ncolumn 7: Plasma temperature (K),\u003Cbr \/\u003E\ncolumn 8: Thermal conductivity (W\/m\/K) for a mixture Ar:H_2=1:1 (Murphy),\u003Cbr \/\u003E\ncolumn 9: Plasma temperature (K),\u003Cbr \/\u003E\ncolumn 10: Thermal conductivity (W\/m\/K) for pure Ar (Murphy),\u003Cbr \/\u003E\ncolumn 11: Plasma temperature (K),\u003Cbr \/\u003E\ncolumn 12: Thermal conductivity (W\/m\/K) for pure H_2 (Murphy).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig14a","mimetype":"text\/csv","size":"21.2 KB","created":"Tue, 10\/04\/2022 - 16:59","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"f427968f-6a06-43b2-bc57-038ab5b22b0e","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig14b.csv","description":"\u003Cp\u003ENet emission coefficient for pure Ar and a mixture 75% Ar + 25% H_2. The data are provided in published works by Menart et al. and Cressault et al.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig14b","mimetype":"text\/csv","size":"5.85 KB","created":"Tue, 10\/04\/2022 - 17:05","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"2e3a05d2-b465-44a8-abcb-6fbb31cbd03a","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig14c_0.csv","description":"\u003Cp\u003EData present a comparison of the computed viscosity against published data (Murphy et al.)\u003Cbr \/\u003E\nDescription of the table:\u003Cbr \/\u003E\ncolumn 1: Plasma temperature (K),\u003Cbr \/\u003E\ncolumn 2: Viscosity (Pa s) for a mixture Ar:H_2=1:1,\u003Cbr \/\u003E\ncolumn 3: Viscosity (Pa s) for a mixture Ar:H_2=1:3,\u003Cbr \/\u003E\ncolumn 4: Viscosity (Pa s) for a mixture Ar:H_2=3:1,\u003Cbr \/\u003E\ncolumn 5: Viscosity (Pa s) for pure Ar,\u003Cbr \/\u003E\ncolumn 6: Viscosity (Pa s) for pure H_2,\u003Cbr \/\u003E\ncolumn 7: Plasma temperature (K),\u003Cbr \/\u003E\ncolumn 8: Viscosity (Pa s) for a mixture Ar:H_2=1:1 (Murphy),\u003Cbr \/\u003E\ncolumn 9: Plasma temperature (K),\u003Cbr \/\u003E\ncolumn 10: Viscosity (Pa s) for pure Ar (Murphy),\u003Cbr \/\u003E\ncolumn 11: Plasma temperature (K),\u003Cbr \/\u003E\ncolumn 12: Viscosity (Pa s) for pure H_2 (Murphy).\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig14c","mimetype":"text\/csv","size":"26.15 KB","created":"Wed, 10\/05\/2022 - 08:45","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"},{"id":"413ae21d-2227-47fc-8653-c7952f1bda83","revision_id":"","url":"https:\/\/www.inptdat.de\/system\/files\/node571_Fig14d.csv","description":"\u003Cp\u003EData provide computed specific heat of pure argon and mixtures of argon with hydrogen.\u003C\/p\u003E\n","format":"csv","state":"Active","revision_timestamp":"Tue, 10\/18\/2022 - 11:14","name":"Effect of a spatially fluctuating heating of particles in a plasma spray process - Fig14d","mimetype":"text\/csv","size":"15.03 KB","created":"Wed, 10\/05\/2022 - 08:57","resource_group_id":"8213480c-adb6-4936-8811-f1dd8f8b3a2f","last_modified":"Date changed  Tue, 10\/18\/2022 - 11:14"}],"tags":[{"id":"f0ab7470-2375-4982-a6ab-55ee5ec67323","vocabulary_id":"2","name":"plasma processing"}],"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"}]}]}