{"data":{"id":"10.6084/m9.figshare.4239215.v1","type":"dois","attributes":{"doi":"10.6084/m9.figshare.4239215.v1","prefix":"10.6084","suffix":"m9.figshare.4239215.v1","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Magdowski, Mathias","nameType":"Personal","givenName":"Mathias","familyName":"Magdowski","affiliation":[],"nameIdentifiers":[]},{"name":"Henning, Gerald","nameType":"Personal","givenName":"Gerald","familyName":"Henning","affiliation":[],"nameIdentifiers":[]},{"name":"Vick, Ralf","nameType":"Personal","givenName":"Ralf","familyName":"Vick","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Measured scattering parameters for the coupling of stochastic electromagnetic fields to an unshielded twisted pair cable with a matched termination for different pitch distances"}],"publisher":"figshare","container":{},"publicationYear":2016,"subjects":[{"subject":"90699 Electrical and Electronic Engineering not elsewhere classified","subjectScheme":"FOR"},{"subject":"FOS: Electrical engineering, electronic engineering, information engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Electrical engineering, electronic engineering, information engineering","subjectScheme":"Fields of Science and Technology (FOS)"}],"contributors":[],"dates":[{"date":"2016-11-18","dateType":"Created"},{"date":"2016-11-18","dateType":"Updated"},{"date":"2016","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsIdenticalTo","relatedIdentifier":"10.6084/m9.figshare.4239215","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["33002658 Bytes"],"formats":[],"version":null,"rightsList":[{"rights":"Creative Commons Attribution 4.0 International","rightsUri":"https://creativecommons.org/licenses/by/4.0/legalcode","schemeUri":"https://spdx.org/licenses/","rightsIdentifier":"cc-by-4.0","rightsIdentifierScheme":"SPDX"}],"descriptions":[{"description":"The coupling of stochastic electromagnetic fields into an unshielded twisted double-wire transmission line has been measured in a reverberation chamber. One end of the line features a matched load resistance and is therefore anechoic. With this chosen configuration, the influence of the pitch distance onto the frequency-dependent coupling can be clearly exposed. The measurement results confirm an existing simulation model that is based on transmission line theory and the plane wave integral representation.\u003cbr\u003e\u003cbr\u003eThe raw data of the measurement is saved in text files.\u003cbr\u003e\u003cbr\u003eEach subfolder is for a different measurement with a different pitch distance or for the coupling between the antennas.\u003cbr\u003e\u003cbr\u003eThe meaning of the examplary filename \"alpha_0.0_s11_imag.out\" is as follows:\u003cbr\u003e- \"alpha_0.0\" stands for a stirrer angle of 0°\u003cbr\u003e- \"s_11\" means the scattering parameter s_11 (there are also s_12, s_21 and s_22)\u003cbr\u003e- \"imag\" is for the imaginary part\u003cbr\u003e- \"real\" is for the real part\u003cbr\u003e\u003cbr\u003eThe content of each file is the scattering parameter, where each line stands for a different frequency.\u003cbr\u003e\u003cbr\u003eThe file \"alphas.out\" contains all the stirrer angles (in °).\u003cbr\u003e\u003cbr\u003eThe file \"freqs.out\" contains all the frequencies (in Hz).\u003cbr\u003e\u003cbr\u003eIf you encounter any problems or if you have any questions, please contact:\u003cbr\u003e\u003cbr\u003eMathias Magdowski\u003cbr\u003eChair for Electromagnetic Compatibility\u003cbr\u003eInstitute for Medical Engineering\u003cbr\u003eOtto von Guericke University Magdeburg, Germany\u003cbr\u003emathias.magdowski@ovgu.de or mathias.magdowski@kabelmail.de\u003cbr\u003eTel. +49-391-67-52195\u003cbr\u003e\u003cbr\u003e\u003cbr\u003e","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://figshare.com/articles/dataset/Measured_scattering_parameters_for_the_coupling_of_stochastic_electromagnetic_fields_to_an_unshielded_twisted_pair_cable_with_a_matche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