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All medical devices should have electromagnetic interference with an electric field strength of 9 V/m to 28 V/m, depending on the frequency range. In this case, these values are too low in relation to the reference levels defined in Recommendation 1999/519/EC, expressed as limits of the intensity of the electric component of the E-field, which are as high as 61 V/m. The presence of electric field strengths higher than 9-28 V/m in the environment may cause negative effects on the operation of medical devices. The negative effects of a medical device are obvious and include damage to human health or even death. This article presents the possibilities of using ferrite absorption material for shielding rooms with medical devices in order to additionally protect them against the limits of the electric component of the E field, which is up to 61 V/m. These values may appear in connection with the currently launched 5G system operating in the high-band frequency range, i.e. 28 GHz and 38 GHz. They may have negative effects on the operation of medical devices. Design/methodology/approach The possibilities of using ferrite absorption material for shielding rooms with medical devices were determined based on the results of measurements of the electrical properties of the ferrite material performed using two methods: the reflection method and the free space method. The article determined the complex electrical permittivity and complex magnetic permeability of a ferrite plate based on measurements of the reflection coefficient and the transmission (attenuation) coefficient. The presented calculation and measurement results were used to show the properties of the ferrite material in the frequency range from 15 GHz to 45 GHz and to show the possibility of using it for shielding rooms as a material absorbing electromagnetic waves in this frequency range. Research limitations/implications The major limitations of the measurement methods used are coaxial probes and measurement antennas, characterised by a limited operating bandwidth. The free space method uses test antennas with a limited operating band of 15-45 GHz. For this reason, the research results were limited to this frequency range. Practical implications The presence of electric field strengths higher than 28 V/m in the environment may cause negative effects on the operation of medical devices. The negative effects of a medical device malfunction are obvious and include damage to human health. The attenuation of the ferrite absorber in the frequency range 15-45 GHz is 16-12 dB, respectively. Therefore, using it as a shielding material in this frequency range will attenuate the electric field intensity from 61 V/m to 10-15 V/m. Since medical devices should be immune to electromagnetic disturbances with an electric field strength of 28 V/m, electric field strengths of 10-15 V/m should not negatively affect their functionality. Originality/value Ferrite absorbers are used in the band from approx. 10 MHz to approx. 1000 MHz. Most often, they are intended for use in anechoic chambers. The publications only provide information on the properties of the ferrite absorber in the frequency range of up to 1 GHz. Due to its properties in the frequency range up to 1 GHz, it was decided to investigate the properties of the ferrite material in the high-frequency range of the 5G system bands, i.e., 28 GHz and 38 GHz, to show the properties of this material and the possibility of using it in these frequency ranges as a shielding material. The properties of the ferrite absorber in the presented frequency band are not published.
Wydawca
Rocznik
Tom
Strony
247--257
Opis fizyczny
Bibliogr. 24 poz., rys.
Twórcy
autor
- Department of Electronics, Military University of Technology, ul. Gen. Sylwestra Kaliskiego 2, 00-908 Warszawa, Poland
autor
- Department of Electronics, Military University of Technology, ul. Gen. Sylwestra Kaliskiego 2, 00-908 Warszawa, Poland
Bibliografia
- [1] S. Kazuo, K. Ishizuka, M. Tokuda, A Study of RF Absorber for Anechoic Chambers Used in the Frequency Range for Power Line Communication System, Piers Online 2/5 (2006) 538-543.
- [2] I. Araz, The measurement of shielding effectiveness for small-in-size ferrite-based flat materials, Turkish Journal of Electrical Engineering and Computer Sciences 26/6 (2018) 18. DOI: https://doi.org/10.3906/elk-1803-162
- [3] M.H. Zahari, B.H. Guan, E.M. Cheng, M.F.C. Mansor, K.C. Lee, EMI Shielding Effectiveness of Composites Based on Barium Ferrite, PANI, and MWCNT, Progress in Electromagnetics Research 52 (2016) 79-87. DOI: https://doi.org/10.2528/PIERM16080701
- [4] IEC 61000-4-3:2020; Part 4-3: Testing and Measurement Techniques - Radiated, Radio-Frequency, Electromagnetic Field Immunity Test. Electromagnetic Compatibility (EMC): Geneva, Switzerland, 2020.
- [5] Council Recommendation 1999/519/EC of 12 July 1999, on the limitation of exposure of the general public to electromagnetic fields (0 Hz to 300 GHz), Official Journal of the European Communities L199 (1999) 0059-0070.
- [6] ICNIRP, Guidelines for limiting exposure to electromagnetic fields (100 kHz to 300 GHz), Health Physics 118/5 (2020) 483-524. DOI: https://doi.org/10.1097/HP.0000000000001210
- [7] IEEE C95.1-2019; IEEE Standard for Safety Levels with Respect to Human Exposure to Electric, Magnetic, and Electromagnetic Fields, 0 Hz to 300 GHz, IEEE, New York, NY, USA, 2019.
- [8] R. Zajicek, L. Oppl, J. Vrba, Broadband Measurement of Complex Permittivity Using Reflection Method and Coaxial Probes, Radioengineering 17/1 (2008) 14-19.
- [9] S.M. Abbas, A.K. Dixit, R. Chatterjee, T.C. Goel, Complex permittivity, complex permeability and microwave absorption properties of ferrite–polimer composites, Journal of Magnetism and Magnetic Materials 309/1 (2007) 20-24. DOI: https://doi.org/10.1016/j.jmmm.2006.06.006
- [10] J. Baker-Jarvis, M.D. Janezic, P.D. Domich, R.G. Geyer, Analysis of an open-ended coaxial probe with lift-off for nondestructive testing, IEEE Transactions on Instrumentation and Measurement 43/5 (1994) 711-718. DOI: https://doi.org/10.1109/19.328897
- [11] S.A. Komarov, A.S. Komarov, D.G. Barber, M.J.L. Lemes, S. Rysgaard, Open-ended coaxial probe technique for dielectric spectroscopy of artificially grown sea ice, IEEE Transactions on Geoscience and Remote Sensing 54/8 (2016) 4941-4951. DOI: https://doi.org/10.1109/TGRS.2016.2553110
- [12] C.E. Kintner, Free-Space Measurements of Dielectrics and Three-Dimensional Periodic Metamaterials, MSc Thesis, University of Arkansas, Fayetteville, 2017. Available from: https://scholarworks.uark.edu/etd/2557
- [13] S. Sahin, N.K. Nahar, K. Sertel, A simplified Nicolson–Ross–Weir method for material characterization using single-port measurements, IEEE Transactions on Terahertz Science and Technology 10/4 (2020) 404-410. DOI: https://doi.org/10.1109/TTHZ.2020.2980442
- [14] A.N. Vicente, G.M. Dip, C. Junqueira, The step by step development of NRW method, Proceedings of the SBMO/IEEE MTT-S International Microwave and Optoelectronics Conference “IMOC 2011”, Natal, Brazil, 2011, 738-742. DOI: https://doi.org/10.1109/IMOC.2011.6169318
- [15] S. Kim, J. Baker-Jarvis, An Approximate Approach to Determining the Permittivity and Permeability Near Lambda/2 Resonances in Transmission/Reflection Measurements, Progress In Electromagnetics Research B 58 (2014) 95-109. DOI: https://doi.org/10.2528/PIERB13121308
- [16] M.-S. Park, J. Cho, S. Lee, Y. Kwon, K.-Y. Jung, New Measurement Technique for Complex Permittivity in Millimeter-Wave Band Using Simple Rectangular Waveguide Adapters, Journal of Electromagnetic Engineering and Science 22/6 (2022) 616-621. DOI: https://doi.org/10.26866/jees.2022.6.r.130
- [17] A.L. de Paula, M.C. Rezende, J.J. Barroso, Modified Nicolson-Ross-Weir (NRW) method to retrieve the constitutive parameters of low-loss materials, Proceedings of the SBMO/IEEE MTT-S International Microwave and Optoelectronics Conference “IMOC 2011”, Natal, Brazil, 2011, 488-492. DOI: https://doi.org/10.1109/IMOC.2011.6169293
- [18] J. Baker-Jarvis, E.J. Vanzura, W.A. Kissick, Improved technique for determining complex permittivity with the transmission/reflection method, IEEE Transactions on Microwave Theory and Techniques 38/8 (1990) 1096-1103. DOI: https://doi.org/10.1109/22.57336
- [19] S.S. Kim, S.B. Jo, K.I. Gueon, K.K. Choi, J.M. Kim, K.S. Churn, Complex permeability and permittivity and microwave absorption of ferrite-rubber composite at X-band frequencies, IEEE Transactions on Magnetics 27/6 (1991) 5462-5464. DOI: https://doi.org/10.1109/20.278872
- [20] K. Hatakeyama, T. Inui, Electromagnetic wave absorber using ferrite absorbing material dispersed with short metal fibers, IEEE Transactions on Magnetics 20/5 (1984) 1261-1263. DOI: https://doi.org/10.1109/TMAG.1984.1063424
- [21] J. Ning, K. Chen, W. Zhao, J. Zhao, T. Jiang, Y. Feng, An ultrathin tunable metamaterial absorber for lower microwave band based on magnetic nanomaterial, Nanomaterials 12/13 (2022) 2135. DOI: https://doi.org/10.3390/nano12132135
- [22] W. Lei, D. ZhiJi, S. JinBiao, Research on broadband graphene composite absorber based on chip electrostatic protection, Proceedings of the 4 th International Conference on Smart Power and Internet Energy Systems “SPIES”, Beijing, China, 2022, 89-93. DOI: https://doi.org/10.1109/SPIES55999.2022.10082126
- [23] R. Araneo, G. Lovat, S. Celozzi, Compact electromagnetic absorbers for frequencies below 1 GHz, Progress in Electromagnetics Research 143 (2013) 67-86. DOI: https://doi.org/10.2528/PIER13070206
- [24] 3M Absorber Sheets Work Below 1 GHz. Available from: https://news.3m.com/2007-05-31-3M-Absorber-Sheets-Work-Below-1-GHz
Typ dokumentu
Bibliografia
Identyfikator YADDA
bwmeta1.element.baztech-de8099ae-5cd7-4de2-a05e-162df931b905
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