{
    "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": "da9b8d93-cc51-4595-a417-35760bef6060",
        "url": "https://www.inptdat.de/node/671",
        "source": {
            "name": "thermal plasma",
            "application": "thermal plasma technology",
            "specification": "DC, atmospheric pressure, thermal",
            "properties": "<p>The model of the free-burning arc in this work employs a tungsten-inert gas arrangement in a 2D axisymmetric computational domain. It includes a La-W cathode with a length of 20 mm, a radius of 2 mm, and a truncated 60\u00b0 conical tip (a plateau radius of 0.2 mm). The anode is a water-cooled copper plate with a radius of 33 mm and a thickness of 7 mm. The distance between the cathode tip and the anode is 8 mm. The arc burns at a direct current of 100 A.</p>\n"
        },
        "medium": {
            "name": "Ar",
            "properties": "<p>The arc burns in atmospheric-pressure argon. The gas is fed with a flow rate of 12 slm through a nozzle with an inner radius of 8 mm.</p>\n"
        },
        "target": [],
        "diagnostics": {
            "name": "method of spherical harmonics, discrete ordinate method",
            "properties": "<p>Simulations are performed applying the net emission coefficient \ud835\udf00\ud835\udc41 (with R = 1 mm), the method of spherical harmonics (first order, P1), and the  and discrete ordinate method (DOM).</p>\n",
            "procedure": "<p>The net emission coefficient (NEC), method of spherical harmonics (P1 as the lowest order), and discrete ordinate method (DOM) methods are implemented into a 2D axisymmetric model of a free-burning arc. Each method requires the knowledge of the radiative properties of the plasma. In the framework of the arc model employing the NEC, the values of the NEC have to be computed prior to the simulation and provided as a function of the temperature. The arc models employing the P1 and the DOM methods make use of a mean absorption coefficient (Planck, Rosseland, hybrid) obtained as a function of the temperature for a number of frequency bands.</p>\n"
        },
        "resource": [
            {
                "id": "8b241791-cd97-484e-ac51-f8d84ea380f7",
                "url": "https://www.inptdat.de/system/files/node671_fig5a_DataI_II_0.csv",
                "filetype": "csv",
                "datatype": "data table",
                "range": "from 300 K up to 30,000 K",
                "quality": "published"
            },
            {
                "id": "f2ea2dfa-3b78-4657-997c-430dbdf2e014",
                "url": "https://www.inptdat.de/system/files/node671_fig5b_DataI_II.csv",
                "filetype": "csv",
                "datatype": "data table",
                "range": "From 300 K up to 30,000 K",
                "quality": "published"
            },
            {
                "id": "1be6f0cb-1a28-4eed-95ce-73aaaae7e051",
                "url": "https://www.inptdat.de/system/files/node671_Fig6a_KappaPRh_DataI_II.csv",
                "filetype": "csv",
                "datatype": "data table",
                "range": "From 300 K up to 30,000 K",
                "quality": "published"
            },
            {
                "id": "c2e60257-011a-4ca2-bfef-2ad3a2384d69",
                "url": "https://www.inptdat.de/system/files/node671_Fig6b_KappaPRh_DataI_II.csv",
                "filetype": "csv",
                "datatype": "data table",
                "range": "From 300 K up to 30,000 K",
                "quality": "published"
            },
            {
                "id": "67d52b9f-690f-4e0b-87cc-7080b0ff682f",
                "url": "https://www.inptdat.de/system/files/node671_Fig10a_NEC_P1_DOM_DataI_II_0.csv",
                "filetype": "csv",
                "datatype": "data table",
                "range": "",
                "quality": "published"
            },
            {
                "id": "714341eb-812e-4ef5-8c81-e3c5e3aa6582",
                "url": "https://www.inptdat.de/system/files/node671_Fig10b_NEC_P1_DOM_DataI_II_0.csv",
                "filetype": "csv",
                "datatype": "data table",
                "range": "",
                "quality": "published"
            },
            {
                "id": "193c6ebb-7721-4fe4-820e-a357069a9523",
                "url": "https://www.inptdat.de/system/files/node671_Fig11a_NEC_P1_DOM_DataI_II_0.csv",
                "filetype": "csv",
                "datatype": "data table",
                "range": "",
                "quality": "published"
            },
            {
                "id": "ab0009aa-0670-40d3-b8b4-412e51c6d45b",
                "url": "https://www.inptdat.de/system/files/node671_Fig11b_NEC_P1_DOM_DataI_II_0.csv",
                "filetype": "csv",
                "datatype": "data table",
                "range": "",
                "quality": "published"
            },
            {
                "id": "73e18561-d12c-484f-846c-57c1f600098e",
                "url": "https://www.inptdat.de/system/files/node671_Fig12_EqTerms_DataI_II_0.csv",
                "filetype": "csv",
                "datatype": "data table",
                "range": "",
                "quality": "published"
            }
        ]
    }
}