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Articles de revues sur le sujet « GTEM »

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Auteur : Grafiati

Publié le 11 septembre 2023

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1

Lee, Soon-Yong, Yeon-Choon Chung et Jea-Hoon Choi. « The Propose of EMI Limits for GETM Cell Using Correlation Factor between OATS and GTEM Cell ». Journal of Korean Institute of Electromagnetic Engineering and Science 22, n^o 1 (31 janvier 2011) : 1–8. http://dx.doi.org/10.5515/kjkiees.2011.22.1.001.

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2

Živković, Zlatko, et Antonio Šarolić. « Measurements of Antenna Parameters in GTEM Cell ». Journal of Communications Software and Systems 6, n^o 4 (22 décembre 2010) : 125. http://dx.doi.org/10.24138/jcomss.v6i4.185.

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The paper presents the method for measuring parameters (gain, antenna factor, impedance and radiation pattern) of small antennas in GTEM cell, which is a novel method and environment for antenna measurements. In order toinvestigate the suitability of GTEM cell for this kind ofmeasurement, the measurement results for a biconical dipole, microstrip patch antennas and small loop antenna were compared with those obtained by calibration inside fully absorber lined anechoic site, two-antenna measurements and FEKO simulations. The measurements were carried out over the wide frequency range. Measurement setup was limited to small antennas that fit into the usable test volume of the GTEM cell. Different sizes that satisfy this restriction were examined. The GTEM measurement results showed considerable agreementwith compared results.

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3

Calò, Giovanna, Francesco Lattarulo et Vincenzo Petruzzelli. « GTEM Cell Experimental Set up for In Vitro Dosimetry ». Journal of Communications Software and Systems 3, n^o 1 (22 mars 2007) : 34. http://dx.doi.org/10.24138/jcomss.v3i1.267.

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A GTEM cell, suitable for assessing possible biological effects induced on cell samples by electromagnetic fields at the typical frequencies of GSM mobile phones, has been designed and set up. Basic environmental requirements for in-vitro biological experiments, involving a GTEM cell, have been assessed by controlling the electromagnetic field distribution and survival conditions. The GTEM cell has been characterized by Standing Wave Ratio (SWR) and Time Domain Reflectometry (TDR) measurements. The impedance matching at the terminal load section has been optimized by considering different hybridload configurations. Moreover, optimal exposure conditions forthe biological sample have been experimentally evaluated by paying special attention to the E-field scenario inside the GTEM cell at 900 MHz and 1800 MHz frequencies. At last, an experimental evaluation of the Specific Absorption Rate (SAR) is reported.

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4

Karsten, U. « Messung der Funkstörfeldstärke mit GTEM-Zellen (Measurements of Disturbance Field Strength using GTEM Cells) ». tm - Technisches Messen 70, n^o 3-2003 (mars 2003) : 113–18. http://dx.doi.org/10.1524/teme.70.3.113.20097.

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5

Suryawijaya, Anita Natalia, Tutiek Purwanti, Djoko Agus Purwanto et Widji Soeratri. « Characteristic and Physical Stability of Anti-Aging Green Tea Extract (GTE) on NLC with Argan Oil as Liquid Lipid ». JURNAL FARMASI DAN ILMU KEFARMASIAN INDONESIA 9, n^o 2 (31 août 2022) : 115–24. http://dx.doi.org/10.20473/jfiki.v9i22022.115-124.

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Background: Green tea extract is a hydrophilic antioxidant that is difficult to penetrate. A nanostructured lipid carrier (NLC) delivers a system consisting of solid-liquid lipids that can improve penetration. Argan oil is a vegetable oil that can be used as a liquid lipid in NLC, reducing particle size and increasing penetration by hydrating the skin. Objective: To determine the formula of NLC green tea extract (NLC-GTE) with liquid lipid argan oil, which has good characteristics and is stable. Methods: Preparation of NLC-GTE used the High Shear Homogenization with solid lipids (cetyl palmitate-glyceryl stearate) - liquid lipids (argan oil) NLC-GTE1 (50:50), NLC-GTE2 (70:30), and NLC-GTE3 (90:10). Characteristic tests included organoleptic, pH, particle size (PS), and polydispersity index (PI). The physical stability test (organoleptic, pH, PS, and PI) used the thermal cycling method (3 cycles six days). Result: NLC-GTE1 – NLC-GTE2 has an odor of argan oil. NLC-GTE3 has odorless. NLC-GTE1 – NLC-GTE3 has a pH scale from 5.782-5.784; PS ranges from 359.73–432.56 nm; PI ranges from 0.175-0.257. The statistical analysis results showed no significant difference between NLC-GTE1 – NLC-GTE3 in pH and PI, there was a significant difference in PS NLC-GTE1; NLC-GTE2 against NLC-GTE3. Physical stability test NLC-GTE2 – NLC-GTE3 phase separation occurs. The statistical analysis results showed no significant difference in pH values NLC-GTE1 – NLC-GTE3 before and after storage; there was a significant difference in NLC-GTE3 before and after storage. Conclusion: NLC-GTE1 was a formula with good characteristics and stability.

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6

Lee, S. U., H. J. Eom et J. H. Kwon. « TEM Mode in the GTEM Cell ». Journal of Electromagnetic Waves and Applications 25, n^o 4 (janvier 2011) : 519–26. http://dx.doi.org/10.1163/156939311794500296.

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7

De Leo, R., T. Rozzi, C. Svara et L. Zappelli. « Rigorous analysis of the GTEM cell ». IEEE Transactions on Microwave Theory and Techniques 39, n^o 3 (mars 1991) : 488–500. http://dx.doi.org/10.1109/22.75291.

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8

Sun, Xiao Ning, Qing Guo Wang et Xing Zhou. « Research on Response of Log-Periodic Antenna (LPDA) to Square Wave Pulse in GTEM Cell ». Applied Mechanics and Materials 556-562 (mai 2014) : 1687–90. http://dx.doi.org/10.4028/www.scientific.net/amm.556-562.1687.

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In order to study the response of the log-periodic antenna (LPDA) to a square wave pulse, it has been irradiated in a square wave pulse using GTEM cell and high-frequency noise generator. And the waveform and frequency spectrum signals are measured. Before the test, the pulse field in GTEM cell has been calibrated. The results showed that field intensity in it changes with the voltage varies linearly strictly at the same point, but with the height of core plate increases, the field intensity decays exponentially but not strictly linear attenuation relationships. Experiment results show that it is feasible to acquire antenna’ square wave pulse response using GTEM cell, and the results is instructive for the analysis of the impulse response and protection for a log-periodic antenna.

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9

Thye, H., G. Armbrecht et M. Koch. « Transient measurement results of pulse propagation in large GTEM cells ». Advances in Radio Science 6 (26 mai 2008) : 307–10. http://dx.doi.org/10.5194/ars-6-307-2008.

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Abstract. This contribution deals with the results of a transient measurement campaign incorporating ultra-wideband (UWB) pulses applied to a large GTEM cell. The main purpose is to analyse the distortion effects on such a feeding pulse when transformed into a field pulse inside the cells testing volume. We will investigate if the TEM field distribution is interfered by multimode propagation, that may lead to location-dependent pulse distortion and ringing. Finally, conclusions on the applicability of GTEM cells for standardized transient EMC measurements will be drawn.

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10

Muterspaugh, M. W. « Measurement of indoor antennas using GTEM cell ». IEEE Transactions on Consumer Electronics 49, n^o 3 (août 2003) : 536–38. http://dx.doi.org/10.1109/tce.2003.1233768.

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11

Nothofer, A., et A. C. Marvin. « Aspects of GTEM to oats measurement correlation ». Computer Standards & ; Interfaces 20, n^o 6-7 (mars 1999) : 484. http://dx.doi.org/10.1016/s0920-5489(99)91096-6.

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12

Narang, Naina, Satya K. Dubey et V. N. Ojha. « Numerical Analysis and Measurement of Electric field Strength inside GTEM Cell at GSM Frequencies ». Defence Science Journal 69, n^o 5 (17 septembre 2019) : 423–26. http://dx.doi.org/10.14429/dsj.69.14944.

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A miniaturised gigahertz transverse electromagnetic (GTEM) cell is designed and fabricated to generate uniform electric (E-) field, essential for studying the radio frequency exposure effect on tissue equivalent liquids at global system for mobile (GSM) communication frequencies (914 MHz and 2.10 GHz). The simulation procedure is discussed and its results are compared with measurement data. The E-field strength inside the GTEM cell is scanned using a microstrip based E-field probe and complete uncertainty evaluation procedure is discussed. Theoretically, simulated and measured E-field strength is reported with expanded uncertainty.

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13

Nain, Caroline Waingeh, Eric Mignolet, Marie-France Herent, Joëlle Quetin-Leclercq, Cathy Debier, Melissa M. Page et Yvan Larondelle. « The Catechins Profile of Green Tea Extracts Affects the Antioxidant Activity and Degradation of Catechins in DHA-Rich Oil ». Antioxidants 11, n^o 9 (19 septembre 2022) : 1844. http://dx.doi.org/10.3390/antiox11091844.

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This study investigated the effect of the catechins profile on the antioxidant activity of green tea extracts (GTEs) by comparing the antioxidant activity of an EGC-rich GTE (GTE1, catechin content: 58% EGC, 30.1% EGCG, 7.9% EC, and 3.9% ECG) and an EGCG-rich GTE (GTE2, catechin content: 60.6% EGCG, 17.7% EGC, 11.8% ECG, and 9.8% EC) in a DHA-rich oil. The effects of the individual catechins (EGC, EC, EGCG, and ECG) and reconstituted catechins mixtures (CatMix), prepared to contain the same amount of major catechins as in the GTEs, were also measured. All treatments (GTE1, CatMix1, GTE2, CatMix2, EGC250, EC250, EGCG250, and ECG250), each containing epistructured catechins at a concentration of 250 ppm, as well as the control (oil with no added antioxidant), were stored at 30 °C for 21 days with sampling intervals of 7 days. The antioxidant activity was assessed by measuring the peroxide value (PV) and p-anisidine value (p-AV) of oils. Changes in fatty acid content and catechins content were also monitored. Both GTEs enhanced the oxidative stability of the DHA-rich oil, but GTE1 demonstrated a stronger antioxidant activity than GTE2. No significant difference was observed between the PV of treatments with GTE1 and CatMix1 during storage, whereas the PV of oil with GTE2 was significantly higher than that with CatMix2 after 21 days. Among the individual catechins, EGC was the strongest antioxidant. Overall, the antioxidant activities of the extracts and catechins were observed in the decreasing order GTE1 ≈ EGC250 ≈ CatMix1 > GTE2 > EGCG250 ≈ CatMix2 > ECG250 > EC250. A significant change in fatty acid content was observed for the control and EC250 samples, and the catechins were most stable in GTE1-supplemented oil. Our results indicate that the EGC-rich GTE is a more potent antioxidant in DHA-rich oil than the EGCG-rich GTE.

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14

Knobloch, A., et H. Garbe. « Screening attenuation of coaxial cables determined in GTEM-cells ». Advances in Radio Science 2 (27 mai 2005) : 33–38. http://dx.doi.org/10.5194/ars-2-33-2004.

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Abstract. This paper describes the determination of the screening attenuation with a GTEM cell. An analytical part gives the link between the voltage at the cell port and the total radiated power. The next section investigates the optimal cable setup in the cell. With a measurement of the common mode current on the cable and a simulation of the radiation resistance the loop antenna characteristic of the cable setup could be verified. It is shown that the use of ferrit cores decrease the difference between the maximum and the minimum screening attenuation. The determination of great screening attenuation could be improved with the use of N-type measurement cables. A comparison between this GTEM cell method and the standard methods shows a good agreement.

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15

Judd, M. D., et O. Farish. « A pulsed GTEM system for UHF sensor calibration ». IEEE Transactions on Instrumentation and Measurement 47, n^o 4 (1998) : 875–80. http://dx.doi.org/10.1109/19.744636.

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16

Luan, Xiaodong, Qingyun Di, Guoqing Xue et Bin Chen. « Ground-wire Source TEM 3D Full Time Multinary Inversion Using Adaptive Regulation ». Journal of Environmental and Engineering Geophysics 25, n^o 3 (septembre 2020) : 403–13. http://dx.doi.org/10.32389/jeeg19-037.

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Ground-wire source transient electromagnetic method (GTEM) provides better investigation ability than loop source TEM at a given noise level and decay time. However, at the present time, the method still stays in the one-dimensional inversion interpretation stage. Since actual geological structures are three-dimensionally distributed, the three-dimensional electromagnetic forward and inversion are crucial for understanding the electromagnetic responses of complex geological structures. Moreover, the traditional 3D smooth inversions of geophysical data have been found to inaccurately reflect small-scale and isolated anomalies. In this study, a multinary inversion method was introduced and applied to GTEM inversions. It was found that the proposed method had the ability to enable GTEM to more accurately delineate anomalous bodies when applied to detect high-resistivity target. Then, for the purpose of avoiding the need for multiple inversion tests to determine the regularization factors, a self-adaptive scheme was proposed based on the differences between the data fitting functional and the model functional during each iteration step. It was observed that by introducing the multinary inversion with adaptive regulation, more stable and accurate inversion results were obtained. In the current study, the numerical simulation results had successfully verified that the proposed multinary inversion method had provided better resolution than the traditional inversion methods.

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17

Zellerhoff, M., et L. Klinkenbusch. « Numerical analysis of the interaction between a GTEM-cell and a device under test using a hybrid method ». Advances in Radio Science 1 (5 mai 2003) : 49–51. http://dx.doi.org/10.5194/ars-1-49-2003.

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Abstract. Due to the increasing importance of EMC problems through the last years there is a great interest in measurement devices such as GTEM-cells (Giga(Hz)- TEM cells). They promise to allow compact and low-cost emission- as well as susceptibility tests up to very high frequencies. Expensive measurement procedures in open-area test sites or within semi-anechoic chambers would become obsolete in many cases. To estimate the quality and reliability of GTEM-cell measurements it is necessary to have detailed knowledge about the processes within the cell and, in particular, about the interactions between the cell and the DUT (device under test). Due to the high frequency and the cell’s dimensions a purely numerical simulation while using standard techniques such as Finite Element Method, Method of Moments (MoM) or the Finite-Differ-Time-Domain (FDTD) method is inefficient and unnecessary since the GTEM-cell is a mostly empty homogeneous TEM-waveguide. Analytical models allow only the investigation of empty cells. As will be outlined in the following, a suitable way to reduce the numerical complexity of the general problem is the use of a hybrid method, such as the combination of a modal analysis with the MoM.

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18

Смирнов, А. « Применение генераторов плоского поля типа GTEM-камер для радиолокационных измерений ». ELECTRONICS : SCIENCE, TECHNOLOGY, BUSINESS 187, n^o 6 (29 juillet 2019) : 80–83. http://dx.doi.org/10.22184/1992-4178.2019.187.6.80.83.

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Предложен метод измерений эффективной площади рассеяния (ЭПР) объектов с использованием GTEM-камер. Отмечено, что преимущество предложенного подхода состоит в возможности измерений ЭПР в диапазоне частот существенно ниже 0,5–1 ГГц, который недоступен при использовании традиционных средств измерений.

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19

NODA, Akira. « Generalized Transformed Eulerian Mean (GTEM) Description for Boussinesq Fluids ». Journal of the Meteorological Society of Japan. Ser. II 92, n^o 5 (2014) : 411–31. http://dx.doi.org/10.2151/jmsj.2014-501.

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20

Pathak, Hetal M., et Shweta N. Shah. « Volumetric Analysis of GTEM Cell for Wide Frequency Application ». Journal of Physics : Conference Series 1921 (mai 2021) : 012011. http://dx.doi.org/10.1088/1742-6596/1921/1/012011.

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21

Chen *, Z. Y., L. H. Ren, Q. Z. Xue et C. Xu. « Linear method of EMI measurement in a GTEM cell ». International Journal of Electronics 92, n^o 2 (février 2005) : 109–15. http://dx.doi.org/10.1080/00207210500031915.

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22

Borsero, M., G. Vizio, D. Parena et V. Teppati. « Synthetic TDR Measurements for TEM and GTEM Cell Characterization ». IEEE Transactions on Instrumentation and Measurement 56, n^o 2 (avril 2007) : 271–74. http://dx.doi.org/10.1109/tim.2007.890796.

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23

De Leo, R., L. Pierantoni, T. Rozzi et L. Zappelli. « Accurate analysis of the GTEM cell wide-band termination ». IEEE Transactions on Electromagnetic Compatibility 38, n^o 2 (mai 1996) : 188–97. http://dx.doi.org/10.1109/15.494623.

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24

Lee, Woo-Sang. « A Study on the Electromagnetic Modeling and Network Analysis for GTEM Cell Design ». Journal of Korean Institute of Electromagnetic Engineering and Science 19, n^o 7 (31 juillet 2008) : 791–99. http://dx.doi.org/10.5515/kjkiees.2008.19.7.791.

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25

Chung, Yeon-Choon, Sang-Bong Jeon, Suk-Tai Kwun et Jae-Hoon Yun. « Interference Effect of Microwave Oven Noise to Wireless LAN Using a GTEM Cell ». Journal of Korean Institute of Electromagnetic Engineering and Science 20, n^o 3 (31 mars 2009) : 240–47. http://dx.doi.org/10.5515/kjkiees.2009.20.3.240.

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26

Herlemann, H., et M. Koch. « Measurement of the transient shielding effectiveness of shielding cabinets ». Advances in Radio Science 6 (26 mai 2008) : 293–98. http://dx.doi.org/10.5194/ars-6-293-2008.

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Abstract. Recently, new definitions of shielding effectiveness (SE) for high-frequency and transient electromagnetic fields were introduced by Klinkenbusch (2005). Analytical results were shown for closed as well as for non closed cylindrical shields. In the present work, the shielding performance of different shielding cabinets is investigated by means of numerical simulations and measurements inside a fully anechoic chamber and a GTEM-cell. For the GTEM-cell-measurements, a downscaled model of the shielding cabinet is used. For the simulations, the numerical tools CONCEPT II and COMSOL MULTIPHYSICS were available. The numerical results agree well with the measurements. They can be used to interpret the behaviour of the shielding effectiveness of enclosures as function of frequency. From the measurement of the electric and magnetic fields with and without the enclosure in place, the electric and magnetic shielding effectiveness as well as the transient shielding effectiveness of the enclosure are calculated. The transient SE of four different shielding cabinets is determined and discussed.

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27

Bancroft, R. « Measurement of television direct pickup (DPU) in a GTEM cell ». IEEE Transactions on Consumer Electronics 41, n^o 4 (1995) : 1010–13. http://dx.doi.org/10.1109/30.477218.

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28

De Leo, R. « FDTD evaluation of scattering by metallic objects in GTEM cells ». IEE Proceedings - Science, Measurement and Technology 141, n^o 4 (1994) : 287. http://dx.doi.org/10.1049/ip-smt:19941206.

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29

De Leo, R., L. Pierantoni, T. Rozzi et L. Zappelli. « Dipole excitation and scattering by spherical objects in GTEM cell ». IEEE Transactions on Microwave Theory and Techniques 42, n^o 9 (1994) : 1700–1708. http://dx.doi.org/10.1109/22.310565.

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30

Shuguang Xing, Shufang Li, Weijun Hong et Xiaoyang Liu. « Using GTEM Cell to Measure RCS of Electrically Small Scatterers ». IEEE Antennas and Wireless Propagation Letters 10 (2011) : 596–98. http://dx.doi.org/10.1109/lawp.2011.2158795.

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31

PAŁCZYŃSKA, Beata. « Wyniki badań emisji promieniowanej przenośnych baterii akumulatorowych w komorze GTEM ». PRZEGLĄD ELEKTROTECHNICZNY 1, n^o 9 (5 septembre 2017) : 120–25. http://dx.doi.org/10.15199/48.2017.09.24.

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32

Maurice, Olivier, François de Daran, Frédéric Lafon, Rabha Oussedrat et Imad Ben Yacoub. « GTEM cell facility use during project development phases for automotive ». Microelectronics Journal 35, n^o 6 (juin 2004) : 563–69. http://dx.doi.org/10.1016/j.mejo.2003.11.001.

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33

Xing, Shuguang, Xiaode Lv et Chibiao Ding. « Research on input impedance of dipole antenna in GTEM cell ». Journal of Electronics (China) 31, n^o 6 (décembre 2014) : 603–8. http://dx.doi.org/10.1007/s11767-014-4162-y.

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34

Lu, Jing Xia, Fang Dai et Wei Feng Chen. « Performance and Structure of an EMP Simulator ». Applied Mechanics and Materials 220-223 (novembre 2012) : 2027–31. http://dx.doi.org/10.4028/www.scientific.net/amm.220-223.2027.

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The electromagnetic pulse simulator designed in this paper consists of an adjustable direct current high voltage source, a capacitor for energy-storage, an air spark gap switch, a resistive divider for measurement and a GHz transversal electromagnetic wave (GTEM) cell. The analysis model is constructed based on the theory of transmission line. Influencing factors, such as self-load and impedance mismatch of the transmission line (as well as the cell), were analyzed using Pspice. The self-load has the effect of parallel connection with the load of GTEM cell. It may increase the rise-time, decrease the fall time and reduce the voltage peak. The sudden change of the transmission line impedance will make the waveform of pulse contain reflected oscillation. Four types of resistance divider link were also simulated using Pspice. Improper connection of the resistance divider will cause the waveform of pulse oscillation and lengthen the rise-time, which can be reduced by shorting the high voltage lead, using system structure with gradually changing resistance or connecting a damping resistance at the end.

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35

Briest, Niklas, Heyno Garbe et Stefan Potthast. « Extended measurement setup for transient TEM waveguide characterization ». Advances in Radio Science 14 (28 septembre 2016) : 115–20. http://dx.doi.org/10.5194/ars-14-115-2016.

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Abstract. This paper discusses a field measurement method, based on a two-antenna setup, to qualify the transmission of transient signals inside a GTEM cell. The transmission characteristic of the GTEM1250 is evaluated by the Pearson correlation coefficient (PCC) and is presented with a heatmap. Due to deviations of the uncertainty contribution of the field homogeneity, the frequency band around 100 MHz is evaluated and its effect to the PCC is discussed. Therefore, a comparable narrowband transient signal, a damped sinusoidal (DS) is used. Furthermore, a detailed discussion focussing on nonlinear and distorting effects of the GTEM1250 is performed. The measurements in time domain (TD) identify comparable high secondary E-field components in the propagation direction, which are characteristic for higher order modes. Based on the same setup, another measurement is performed in frequency domain (FD) and relates the phase response of the GTEM cell to the above mentioned effects. According to the measured phase response the propagation time is discussed to investigate the distorting effects caused by higher order modes.

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36

Calo, Giovanna, et Vincenzo Petruzzelli. « ELECTROMAGNETIC AND THERMAL ANALYSES OF IMPROVED GTEM CELLS FOR BIOELECTROMAGNETIC EXPERIMENTS ». Progress In Electromagnetics Research 125 (2012) : 503–26. http://dx.doi.org/10.2528/pier11122206.

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37

Malaric, Kresimir, Juraj Bartolic et Roman Malaric. « Immunity measurements of TV and FM/AM receiver in GTEM-cell ». Measurement 38, n^o 3 (octobre 2005) : 219–29. http://dx.doi.org/10.1016/j.measurement.2005.07.010.

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38

Pouhe, D. « RF Radiation Properties of Printed-Circuits Boards in a GTEM Cell ». IEEE Transactions on Electromagnetic Compatibility 48, n^o 3 (août 2006) : 468–75. http://dx.doi.org/10.1109/temc.2006.877778.

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39

Rusiecki, Andrzej. « Impact of the Measurement Setup on Shielding Effectiveness Measurement of Enclosure in GTEM Cell ». Pomiary Automatyka Robotyka 19, n^o 2 (12 mai 2015) : 43–48. http://dx.doi.org/10.14313/par_216/43.

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40

Wu, Ifong, Shinobu Ishigami, Kaoru Gotoh et Yasushi Matsumoto. « Calibration of electric field probes in GTEM cell using reference antenna method ». IEICE Electronics Express 6, n^o 20 (2009) : 1469–75. http://dx.doi.org/10.1587/elex.6.1469.

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41

Kvasznicza, Zoltán, István Gyurcsek, György Elmer, Viktor Bagdán et Ildikó Horváth. « Mathability of EMC Emission Testing for Mission Crucial Devices in GTEM Waveguide ». Acta Polytechnica Hungarica 18, n^o 1 (2021) : 159–73. http://dx.doi.org/10.12700/aph.18.1.2021.1.10.

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42

Zhang, Long, Guanghui Wei, Xiaofeng Hu et Xinfeng Li. « Shielding effectiveness testing method of pulse electric field based on GTEM cell ». Journal of Physics : Conference Series 418 (22 mars 2013) : 012080. http://dx.doi.org/10.1088/1742-6596/418/1/012080.

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43

Lee, Ae-kyoung Lee. « An Advanced Correlation Algorithm between GTEM and OATS for Radiated Emission Tests ». ETRI Journal 17, n^o 3 (1 octobre 1995) : 45–63. http://dx.doi.org/10.4218/etrij.95.0195.0033.

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Kama Huang et Yongqin Liu. « A simple method for calculating electric and magnetic fields in GTEM cell ». IEEE Transactions on Electromagnetic Compatibility 36, n^o 4 (1994) : 355–58. http://dx.doi.org/10.1109/15.328866.

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Ren, Liehui, et Zhiyu Chen. « Improvement of expression for excitation by an electric dipole in GTEM cell ». Journal of Electronics (China) 19, n^o 1 (janvier 2002) : 94–98. http://dx.doi.org/10.1007/s11767-002-0017-z.

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Sahraei, A., et H. Aliakbarian. « On the design and fabrication of a large GTEM cell and its challenges ». IEEE Electromagnetic Compatibility Magazine 9, n^o 1 (2020) : 43–50. http://dx.doi.org/10.1109/memc.2020.9075034.

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Araujo, Humberto X. « A GTEM Chamber Design with Frequency Flexibility Using Metamaterial Concepts on the Septum ». International Journal of Materials Science and Applications 2, n^o 2 (2013) : 47. http://dx.doi.org/10.11648/j.ijmsa.20130202.13.

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No-Weon Kang, Jin-Seob Kang, Dae-Chan Kim, Jeong-Hwan Kim et Joo-Gwang Lee. « Characterization Method of Electric Field Probe by Using Transfer Standard in GTEM Cell ». IEEE Transactions on Instrumentation and Measurement 58, n^o 4 (avril 2009) : 1109–13. http://dx.doi.org/10.1109/tim.2008.2008592.

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Zhang, Weiwei, Wei Zhou, Dongdong Xu, Guangke Xu, Xing Li et Ying Lin. « Research on Electric Field Simulation of GTEM Cell Based on UHF Sensor Calibration ». IOP Conference Series : Earth and Environmental Science 223 (21 janvier 2019) : 012012. http://dx.doi.org/10.1088/1755-1315/223/1/012012.

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Galeev, L. M. « Investigation of the plane wave coupling to a linearly loaded transmission line network ». Power engineering : research, equipment, technology 22, n^o 4 (15 novembre 2020) : 54–63. http://dx.doi.org/10.30724/1998-9903-2020-22-4-54-63.

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Résumé :

The article is concerned with a complex investigation of the influence of the plane wave coupling with a certain function of time, incident direction and polarization to a linearly loaded transmission line network comprised of three single-wire conductors with different lengths connected in the center. Line load is represented as 50 Ω resistors connected to all terminations of the transmission line network. The exemplary network was modeled on a computer and experimentally investigated in a gigahertz transverse electromagnetic GTEM cell, which allows creating an electromagnetic field of a certain direction. The coupled voltage at the terminals of the network was investigated in the frequency and time domains. To conduct an experiment in the frequency domain, both to create an electromagnetic field inside the GTEM camera and to measure the induced voltage at the terminations of the network, a vector network analyzer VNA was used. To conduct an experiment in the time domain for the sake of creating an electromagnetic field, a high-voltage voltage generator was used, whereas a strobing oscilloscope was used to measure the induced voltages. The simulation was performed in the LTspice software - a tool for calculating electrical and electronic circuits, and Matlab. It is also examined to show the compliance with the experimental results. On the basis of obtained results, the author was able to identify the main aspects that may be useful in modeling and predicting the electromagnetic processes occurring in linearly loaded conductors, power supply and / or data transmission systems.

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