Frequency Approach to Analysis of ESD Pulse
|
|
- Dwayne Gray
- 6 years ago
- Views:
Transcription
1 本文は pp Frequency Approach to Analysis of ESD Pulse Janusz Baran Non-member (Czestochowa University of Technology, Poland) Jan Sroka Non-member (EMC-Testcenter Zurich, Switzerland) Keywords : electrostatic discharges, frequency domain analysis, power spectral density, transfer impedance The paper concerns calibration of generators for simulation of the Human-Metal Electrostatic Discharge (ESD) according to the IEC standard. The analysis is restricted to ESD generator current, since only calibration of the current is mandatory in the standard. It is shown that analysis of the ESD pulse in the frequency domain can be an indication if omitting the frequency considerations in calibration of ESD guns is acceptable. The calibration setup (Fig. 1) consists of a target (current converter), attenuator, coaxial cable and a wideband, single shot oscilloscope. It is much easier to use only a low frequency model of such a measurement path setup than consider a high frequency model. If, however, a high frequency treatment is indispensable, then a frequency dependent transfer impedance of the measurement path (Fig. 2) and approximation of the oscilloscope frequency response with an infinite impulse response discrete time filter are adequate tools, because the distortion of a recorded pulse due to frequency characteristic of the instrumentation has to be taken into consideration. Comparison of power spectral densities (PSD) of theoretical pulses, measured pulses (Fig. 3) as well as the measurement path noise (Fig. 4) gives a good criterion for specifying minimal bandwidth of a setup required for reliable calibration of a given ESD gun. The main conclusions of the paper are as follows: 1) a measurement path with a 3 GHz bandwidth is sufficient to neglect ESD Gen. target (current converter) cable with attenuator OSC Fig. 1. Setup for ESD pulse calibration Fig. 2. Transfer impedance of the calibration path versus frequency Fig. 3. Normalized ESD pulses of the same ESD gun (series of 6 measurements, 6 GHz oscilloscope bandwidth) along with theoretical approximations: a) waveforms, b) PSD spectra Fig. 4. Approximately flat PSD of measurement noise calculated for initial 1 ns interval prior to start of the pulses from Fig. 3 frequency distortions for the theoretical pulse with a.6 ns rise time the fastest allowable by the IEC standard, 2) if a real ESD pulse is relatively smooth, the main component of its spectrum above 3 GHz is the noise, whose source is the gun s discharge switch. If the spectrum of a real pulse compared to the noise is limited to below 2 GHz, it is distorted in principle in the same way as a clean theoretical pulse. A too narrow bandwidth, especially less than 1. GHz, can easily result in incorrect evaluation of the metrics and erroneous verdict of verification. When a setup bandwidth is greater than 2 GHz, the main source of the measurement uncertainty becomes the pulse noise, which can be reduced by averaging over a series of pulses. Even though a 3 GHz bandwidth setup does not ensure distortion-free transmission of a pulse, further expansion of an oscilloscope bandwidth will not reduce the deterministic component of the uncertainty. Verification of guns that produce rough pulses, with steps on the rising slope and/or several smaller peaks, whose high frequency part of the spectrum above 3 GHz contains distinctive resonance peaks emerging above the noise level, requires a wider bandwidth 4 GHz or even more. The paper is a resume of previous papers of the authors, in which these issues were presented in details. -1-
2 本文は pp Measurement of Radiated Electromagnetic Field due to Low Voltage ESD with Spherical Electrode in 1-3GHz Frequency Bandwidth Ken Kawamata Senior Member (Hachinohe Institute of Technology) Shigeki Minegishi Senior Member (Tohoku Gakuin University) Osamu Fujiwara Senior Member (Nagoya Institute of Technology) Keywords : ESD, micro gap discharge, low voltage discharge, electromagnetic noise, radiation, spherical electrode 1. Introduction The very fast transients are arisen by gap discharges with low voltage ESD (electrostatic discharges). The low voltage ESD has very wideband (high frequency) electromagnetic noise source. Over the past few years a considerable number of studies have been made on electromagnetic noises of ESD from the point of view of the EMC (electromagnetic compatibility). The electromagnetic noise characteristics of the gap discharges are gradually becoming clearer. In this paper, the amplitude properties of radiated electromagnetic field due to low voltage ESD were examined by experimental study. We present an experimental system to measure the radiated electromagnetic filed in wideband region from 1GHz to 3GHz frequency bandwidth using a pair of spherical electrode and a horn antenna. 2. Experimental System and Experiments Figure 1 shows an experimental system using spherical electrodes and a horn antenna for the wideband measurements. The system consists of a high voltage D.C. power supply, a pair of spherical electrodes, high resistance lines, a horn antenna (ETS 311, 1-18GHz), an attenuator of 1dB and digitizing oscilloscope (Tektronix TDS694C, 3GHz, 1GS/s). In this experiment, four pairs of diameter electrodes were used to measure the radiated electromagnetic field. The type (a) is a pair of 12.8mm diameter electrodes, Type (b) is 19.mm, Type (c) is 2.mm, and Type (d) is 3.mm. These electrodes were made by brass ball. In the experiment, a constant voltage applies to the electrode, a gap length between the electrode decreases slowly about 1 cm/s. The amplitude of received electromagnetic field was measured by the oscilloscope when discharge occurred. The discharge voltage is from 3V to 6V. The amplitude of received electromagnetic field was expressed by a peak to peak value of received voltage measured by digitizing oscilloscope. 3. Experimental Results Figure 2 shows relationship between the discharge voltage and the received voltage. The received voltage shows an average value of more than a hundred measurements. The diamond marks indicate the relation in the type (d), the square marks are type (c), the triangular marks are type (b), and circle marks are type (a). In overall, the received voltage has proportional relation to the discharge voltage from 3V to 62V in each electrode. However, the received voltage is not proportion to discharge voltage in more than 63V discharge, respectively. And so, received voltage showed a same tendency between the type (a), (b), (c), and (d). The amplitude of radiated electromagnetic field has a widely variation of amplitude in high voltage discharge more than 63V. Furthermore, the received voltage was proportion to the diameter of the spherical electrode in the wideband experimental system. Oscilloscope Oscilloscope (Tek. TDS694C, 3GHz) Double Rigid Guide Horn Antenna ETS 311,1-18GHz Spherical Electrodes (Diameter is 3 mm) Received Voltage V [Vp-p] High Resistance kω Tek. TDS694C, 3GHz Attenuator 1dB Coaxial line (D2W, 3m) 1m Feed line. (High resistance line) High Voltage D.C. Power Supply. (1V-1V) Fig. 1. Measurement system for amplitude of the radiated EM field due to discharge using a pair of spherical electrode and a horn antenna Type (a):12.8mm Type (d):3.mm Type (c):2.4mm Type (b):19.mm Discharge Voltage [V] Fig. 2. Relationship between discharge voltage and received voltage of radiated electromagnetic field 4. Conclusion As a result, the amplitude of radiated electromagnetic field is proportion to the discharge voltage from 3V to 62V, and the amplitude of radiated electromagnetic field was proportion to diameter of the spherical electrode in the wideband system. -2-
3 本文は pp.3-3 Measurement and Validation of Transfer Impedance of IEC Calibration Current Target for Electrostatic Discharge Generators Yukio Yamanakai Member (National Institute of Information and Communications Technology, Takashi Adachi Non-member (Nagoya Institute of Technology) Shinobu Ishigami Member (National Institute of Information and Communications Technology) Ikuko Mori Non-member (Suzuka College of Technology) Yoshinori Taka Member (Kushiro College of Technology) Osamu Fujiwara Senior Member (Nagoya Institute of Technology) Keywords : electrostatic discharge generators, IEC calibration current target, transfer impedance, injection current, reconstruction The electrostatic discharge (ESD) events due to charged human bodies produce electromagnetic (EM) fields having broad-band frequency spectra, which cause malfunctions in high-tech information equipment. In this context, the International Electrotechnical Commission (IEC) prescribes the ESD immunity test (IEC61-4-2) of electronic equipment, and specifies the detailed waveform of a discharge current injected onto the IEC recommended calibration current target in contact with an ESD generator, which is designed to have a transfer impedance (rate to a sinusoidal current injected of its observed sinusoidal voltage onto the target) of 1 Ω so that the waveforms of an injected current and the resultant observed output voltage coincide at low frequencies. Due to its frequency characteristics, however, in the high frequency range, the observed voltage waveform does not correspond to the injected current one. In the present study, using a Ω tapered coaxial type adapter and a S-parameter technique, we measured the transfer impedance of a commercially available IEC calibration current target used for the immunity testing against ESDs, and thereby reconstruct the waveforms of discharge currents injected onto the target from their observed output voltages for contact and air discharges of an ESD generator. Figures 1 and 2 show a setup for measuring scattering parameters of an IEC calibration current target and the measured result of the transfer impedance, respectively. We found that the transfer Port1 N-type connecter Network analyzer Port2 Ω coaxial cable Calibration adapter Calibration target Calibration plane N-type connecter Fig. 1. Setup for measuring scattering parameters of IEC calibration current target Z T (jω) [Ω] Real Part Imaginary Part Z T (jω) 1 Ω Ω Frequency [MHz] Fig. 2. Measured frequency characteristics of transfer impedance v o (t) [V], i(t) [A] t r = 8 ps t r = ps t r = 1 ps Observed voltage voltage Reconstructed Estimated current Charge voltage = 4kV 2kV.kV Time t [ns] Fig. 3. Observed voltages and reconstructed discharge currents injected on the target for air discharges with slow approach impedance is almost 1+j Ω at frequencies below 1 GHz, while due to resonance phenomena occurring at frequencies around 2 GHz and GHz, resistive and reactive components significantly change at frequencies over 1 GHz, though their absolute values are slightly larger than 1 Ω. Figure 3 shows observed output voltages and reconstructed discharge currents injected on the target for air discharges with slow approach, which demonstrates that the reconstructed discharge currents agree well with the observed voltages with rise time of ps and 8 ps, while in the case for the observed voltage with a rapid rise time of 1 ps, the reconstructed current has a slightly small peak and a bit gentle rise time in comparison with those of the observed voltages due to the resonance characteristics of the transfer impedance at frequency over 1 GHz. -3-
4 本文は pp Measurement of Leaked High-Frequency Burst Electric Field and EMI Evaluation for Cardiac Pacemaker in Fusion Facility Yukio Yamanaka Member (National Institute of Information and Communications Technology, Jianqing Wang Non-member (Nagoya Institute of Technology, Osamu Fujiwara Senior member (Nagoya Institute of Technology, Tatsuhiko Uda Non-member (National Institute for Fusion Science, Keywords : fusion experimental facility, leaked electromagnetic field, statistical distribution, electromagnetic interference In the fusion facility, many devices such as plasma heating and discharge cleaning leak electromagnetic fields with an irregular variation ranging from several MHz to several hundred GHz. The objective of this study is to quantify the special electromagnetic environment and evaluate its safety for workers. We first measured the electric field leaked from a heating device in the ion cyclotron range of high-frequency (ICRF). The signal from the ICRF is amplified with a two-stage amplifier at frequencies of 3 1 MHz, and is then sent to a plasma load through a waveguide. Using a real time spectrum analyzers (Tektronix RSA338B) together with a bi-conical antenna, we measured the time variation and spectrum of the leaked electric field in the vicinity of the amplifier of ICRF for the plasma load. The real time spectrum analyzer can record the time waveform and the spectrum of measured electric field at the same time through a Fourier transform hardware. As a result, as shown in Fig. 1, the leaked electric field was in a burst form with a varying field level and the center frequency was at 38. MHz with most of energies ranging within ±2 MHz. Within each burst period, we extracted the amplitude probability distribution (APD) and the crossing rate distribution (CRD). Figure 2 shows an example of the possibility density function (PDF) of the leaked electric field. It is much different from a normal distribution, and consequently the mean value of electric field differs from the median value and Electric E field field [V/m] [V/m] Frequency [MHz] 電界 vs. 時間 Time [s] x 1 Time [s] Fig. 1. Spectrum and time variation of leaked electric field in one burst period the mode value. The leaked electric field itself also varied violently with time, reached 4 times in one second to cross the mode value of the leaked electric field. Yet, although the electric field varies with time in a burst form, its maximum level did not exceed 1 V/m. Under such an electric field level environment, the SAR is always much smaller than the ICNIRP safety guideline for any type of statistical variations. In addition, we also evaluated the possibility of electromagnetic inference (EMI) to an implanted cardiac pacemaker in the measured electromagnetic environment. We employed a nonlinear operational amplifier model with Volterra series representation to predict the output voltage of the sensing circuit of pacemaker which consists of an amplifier and a low-pass filter. Using the measured voltage in the real time spectrum analyzer as the input to the sensing circuit as a worst case, we found that the interference voltage induced in the output of the pacemaker sensing circuit did not exceed the threshold for a malfunction. As shown in Table 1, due to the narrow bandwidth of the leaked signal, only using the leaked electric field at the center frequency was sufficient for this EMI evaluation. Probability density [%] Density X18z data E field [V/m] Electric field [V/m] Fig. 2. Probability density of leaked electric field in one burst period Table 1. Relationship between the DC offset output voltage and bandwidth BW [MHz] Vout DC [mv] Difference.87.% % % -4-
5 本文は pp Waveform Distortion of Discharge Rising Currents caused by Built-in Inductor for Contact Discharges of Electrostatic Discharge Generators Yukio Yamanakai Member (National Institute of Information and Communications Technology, Fumihiko Toya Non-member (Nagoya Institute of Technology) Shinobu Ishigami Member (National Institute of Information and Communications Technology) Osamu Fujiwara Senior Member (Nagoya Institute of Technology) Keywords : electrostatic discharge generator, contact discharge, discharge current, built-in inductor, waveform distortion The International Electrotechnical Commission (IEC) prescribes an immunity test (IEC61-4-2) of electronic equipment for electrostatic discharges (ESDs), and specifies not the whole-waveform but only the rise time, the first peak, the levels at 3 ns and 6 ns of a discharge current injected by an electrostatic discharge generator (ESD gun) onto an IEC recommended calibration target. The rise time is required to be.8 ns ±2 %, which can commonly be realized by mounting an inductor in series with a metal electrode for current injection. Due to the impedance of the inductor, however, discharge currents should rise not smoothly but deformedly, which can affect immunity test results. In this study, to investigate the effects of built-in inductors of ESD guns on current rising waveform, we simultaneously measured discharge currents and the resultant magnetic near-fields for contact discharges of an ESD-gun, and compared their results with those for an ESD-gun with a metal cylinder in lieu of the inductor. Figure 1 shows the configuration and structure of a built-in inductor of an ESD gun and the same sized metal cylinder used in place of the inductor. Figure 2 shows an example for the waveforms of output voltages induced in a magnetic field probe for contact discharges of the ESD gun with a built-in inductor. Tip electrode for discharge With a plastic cover Without a plastic cover 22. mm 1mm Gun body 9 mm 8 mm (a) Configuration of built-in inductor 22. mm (b) Built-in inductor 9 mm 22. mm 8 mm (c) Metal cylinder (brass) Fig. 1. (a) Configuration and structure of built-in inductor, (b) dimension of built-in inductor and (c) the same sized metal cylinder of ESD gun Also shown in the same figure is the result for the metal cylinder in place of the built-in inductor. As a result, we found that the magnetic near-field waveform is deformed by the distortion of the current rising waveform for an ESD-gun with an inductor, while the ESD gun with a metal cylinder produces no distortion for the current rising waveform despite its rise time (4 ps) shorter than the IEC specification so that there is no distortion for the corresponding magnetic near-field waveform. Using the Heidler s formula for typical discharge current waveform specified in the IEC, we calculated current rising waveform and the resultant induced output voltage of a magnetic probe, which shows that these results do not agree with those for the built-in inductor, while there is good agreement for the metal cylinder. This finding implies that immunity test results can be affected by the frequency characteristics of a built-in inductor inside an ESD gun, and thus that not only rise time but also current rising waveform of a discharge current should be specified for ESD immunity testing. Measured (a) (b) Observed voltage v o (t) [V] 1 Z = [Ω] d=13 mm v o (t) Z = [Ω] d=13 mm Charge voltage = 2 kv Calculated from measured current Calculated from Heidler s current Time t [ns] v o (t) Time t [ns] Fig. 2. Waveforms of output voltages induced in magnetic field probe for contact discharge of ESD gun with (a) built-in inductor and (b) metal cylinder installed in place of built-in inductor --
6 本文は pp Measurement Method for Impulse Electromagnetic Field by Half TEM Horn Tsubasa Tachibana Non-member (Tohoku Gakuin University) Ken Kawamata Senior Member (Hachinohe Insitute of Technology) Shigeki Minegishi Senior Member (Tohoku Gakuin University) Keywords : Half TEM Horn, impulse electoromagnetic field, ESD 1. Introduction The measuring method of impulse electromagnetic field by Half TEM Horn elctoromagnetic fieid generator (EM generator) and Half TEM Horn electoromagnetic field detector (EM detector) was proposed. The impulse electromagnetic field is generated between the ground plane and element of EM generator and is detected by EM detector inserted in EM generator. As a result of the TDR experiment of EM generator and EM detector, the characteristic impedance from the input to the aperture was fixed Ω. As a result of the experiment of impulse (Amplitude 16mV, Pulse width 63ps) response, the received electric power was proportional to the cross section of the aperture of the EM detector and the received pulse width was almost invariable to the cross section of the aperture of the EM detector. This method enables the measurement which decreases the amplitude without changing the pulse width of strong impulse electromagnetic field due to the discharge such as ESD. 2. As a Result of Experiment Figure 1 shows the measurement system of the impulse electromagnetic field which is generated between the ground plane and element of EM generator and is detected by EM detector inserted in EM generator. Figures 2 and 3 show the results of experiments. The received electric power was proportional to the cross section of the aperture of the EM detector in Fig. 2. The received pulse width was almost invariable to the cross section of the aperture of the EM detector in Fig Conclusion This method enables the measurement which decreases the amplitude without changing the pulse width of strong impulse electromagnetic field due to the discharge such as ESD. (a) Top view Fig. 2. Relation between S out /S in and P out /P in at θ=3, 4, (b) Longitudinal section Fig. 1. Experimental system Fig. 3. Relation between τ out /τ in and S out /S in at θ=3, 4, -6-
7 本文は pp Fundamental Study on Mechanism of Electromagnetic Field Radiation from Electric Devices with Loose Contact of Connector Keywords : contact failure, SMA connector, common-mode current Kazuki Matsuda Non-member (Tohoku University) Yu-ichi Hayashi Member (Tohoku University) Takaaki Mizuki Non-member (Tohoku University) Hideaki Sone Member (Tohoku University) 1. Introduction When a connector is tightened with insufficient torque, electromagnetic field radiation from interconnected devices is increased. To elucidate the mechanisms of electromagnetic field radiation due a loose connector contact, we investigate the high-frequency circuit elements at the contact boundary. From the experimental results, we show the relationship between the high-frequency circuit elements and the electromagnetic field radiation from electric devices. 2. High-frequency Circuit Elements at Contact Boundary In this experiment, to investigate high-frequency circuit elements at the contact boundary of a loose connector, we employ time domain reflectometry (TDR). The measurement setup is shown in Fig. 1. The rise time of the input step pulse is 1. ns, and the voltage is 1. V. Figure 2 shows the measurement results. The peak voltage is higher for insufficient torque (dashed line) than for sufficient torque (solid line). Therefore, the inductance at the contact boundary is increased by loosening the connector. In addition, the level of reflected voltage after the peak is higher for insufficient torque (dashed line) than for sufficient torque. This finding indicates that the resistance at the contact boundary is increased by loosening the connector. The inductance and resistance at the connector boundary are both increased when the connector is tightened with insufficient torque. 3. Relationship of L and R with Common-Mode Current In this section, we show the relationship of electromagnetic field radiation with the difference, due to tightening (torque), in inductance ( L) and resistance ( R). L and R, respectively, are Fig. 1. Measurement setup for TDR Fig. 2. Measurement results for TDR Fig. 3. Measurement results for common-mode current (a) Relationship of L with CM (b) Relationship of R with CM Fig. 4. Relationships of L and R with CM the differences after tightening from L and R at the base torque (.6 N m). In this experiment, we perform electromagnetic field radiation measurement at the same time as TDR. We employ the same TDR procedure as described in Section 2. Common-mode (CM) current is measured because it is one of the main factors in electromagnetic field radiation. The measurement setup consists of a spectrum analyzer in place of an oscilloscope, and a current probe is placed at positions along a semi-rigid cable. Measurement results for CM current are shown in Fig. 3. The relationships of L and R with CM current are shown in Fig. 4: CM L and CM R. The increase in CM current depends on frequency when only the inductance at the contact boundary is increased, but not when only the resistance of the contact boundary is increased. 4. Conclusion The results show that the inductance and resistance at a contact boundary are increased by loosening the connector: specifically, we found that CM L and CM R. Moreover, the increase in inductance has a large effect on the increase in CM current. -7-
TRANSFER IMPEDANCE MODEL OF MEASUREMENT PATH FOR ESD SIMULATOR CALIBRATION
EMC 6 8 th INERNAIONAL WROCLAW SMPOSIUM AND EXHIBIION ON ELECROMAGNEIC COMPAIBILI, WROCLAW, 8 3 JUNE, 6 www.emc.wroc.pl RANSFER IMPEDANCE MODEL OF MEASUREMEN PAH FOR ESD SIMULAOR CALIBRAION Janusz Baran,
More informationMeasurement Notes. Note 53. Design and Fabrication of an Ultra-Wideband High-Power Zipper Balun and Antenna. Everett G. Farr Farr Research, Inc.
Measurement Notes Note 53 Design and Fabrication of an Ultra-Wideband High-Power Zipper Balun and Antenna Everett G. Farr Farr Research, Inc. Gary D. Sower, Lanney M. Atchley, and Donald E. Ellibee EG&G
More informationComparison of IC Conducted Emission Measurement Methods
IEEE TRANSACTIONS ON INSTRUMENTATION AND MEASUREMENT, VOL. 52, NO. 3, JUNE 2003 839 Comparison of IC Conducted Emission Measurement Methods Franco Fiori, Member, IEEE, and Francesco Musolino, Member, IEEE
More informationSpecification. CTR 2 ESD calibration target
Specification CTR 2 ESD calibration target IEC 61000-4-2 IEC 61000-4-2 77B/378/CDV ISO CD 10605 N1347 The CTR 2 is a coaxial current target to monitor Electro Static Discharges as required in the draft
More informationSaturation of Active Loop Antennas
Saturation of Active Loop Antennas Alexander Kriz EMC and Optics Seibersdorf Laboratories 2444 Seibersdorf, Austria Abstract The EMC community is working towards shorter test distances for radiated emission
More informationEffectively Using the EM 6992 Near Field Probe Kit to Troubleshoot EMI Issues
Effectively Using the EM 6992 Near Field Probe Kit to Troubleshoot EMI Issues Introduction The EM 6992 Probe Kit includes three magnetic (H) field and two electric (E) field passive, near field probes
More informationProgress In Electromagnetics Research, Vol. 119, , 2011
Progress In Electromagnetics Research, Vol. 119, 253 263, 2011 A VALIDATION OF CONVENTIONAL PROTECTION DEVICES IN PROTECTING EMP THREATS S. M. Han 1, *, C. S. Huh 1, and J. S. Choi 2 1 INHA University,
More informationAC Current Probes CT1 CT2 CT6 Data Sheet
View at www.testequipmentdepot.com AC Current Probes CT1 CT2 CT6 Data Sheet Features & Benefits High Bandwidth Ultra-low Inductance Very Small Form Factor Characterize Current Waveforms up to
More informationSignal and Noise Measurement Techniques Using Magnetic Field Probes
Signal and Noise Measurement Techniques Using Magnetic Field Probes Abstract: Magnetic loops have long been used by EMC personnel to sniff out sources of emissions in circuits and equipment. Additional
More informationTrees, vegetation, buildings etc.
EMC Measurements Test Site Locations Open Area (Field) Test Site Obstruction Free Trees, vegetation, buildings etc. Chamber or Screened Room Smaller Equipments Attenuate external fields (about 100dB) External
More informationTransient calibration of electric field sensors
Transient calibration of electric field sensors M D Judd University of Strathclyde Glasgow, UK Abstract An electric field sensor calibration system that operates in the time-domain is described and its
More informationAn Analysis of the Fields on the Horizontal Coupling Plane in ESD testing
An Analysis of the Fields on the Horizontal Coupling Plane in ESD testing Stephan Frei David Pommerenke Technical University Berlin, Einsteinufer 11, 10597 Berlin, Germany Hewlett Packard, 8000 Foothills
More informationCorrelation Between Measured and Simulated Parameters of a Proposed Transfer Standard
Correlation Between Measured and Simulated Parameters of a Proposed Transfer Standard Jim Nadolny AMP Incorporated ABSTRACT Total radiated power of a device can be measured using a mode stirred chamber
More informationCHAPTER 6 EMI EMC MEASUREMENTS AND STANDARDS FOR TRACKED VEHICLES (MIL APPLICATION)
147 CHAPTER 6 EMI EMC MEASUREMENTS AND STANDARDS FOR TRACKED VEHICLES (MIL APPLICATION) 6.1 INTRODUCTION The electrical and electronic devices, circuits and systems are capable of emitting the electromagnetic
More informationEMC standards. Presented by: Karim Loukil & Kaïs Siala
Training Course on Conformity and Interoperability on Type Approval testing for Mobile Terminals, Homologation Procedures and Market Surveillance, Tunis-Tunisia, from 20 to 24 April 2015 EMC standards
More informationElectromagnetic Compatibility
Electromagnetic Compatibility Introduction to EMC International Standards Measurement Setups Emissions Applications for Switch-Mode Power Supplies Filters 1 What is EMC? A system is electromagnetic compatible
More informationTechniques to reduce electromagnetic noise produced by wired electronic devices
Rok / Year: Svazek / Volume: Číslo / Number: Jazyk / Language 2016 18 5 EN Techniques to reduce electromagnetic noise produced by wired electronic devices - Tomáš Chvátal xchvat02@stud.feec.vutbr.cz Faculty
More informationExperimental Observation of RF Radiation Generated by an Explosively Driven Voltage Generator
Naval Research Laboratory Washington, DC 20375-5320 NRL/FR/5745--05-10,112 Experimental Observation of RF Radiation Generated by an Explosively Driven Voltage Generator MARK S. RADER CAROL SULLIVAN TIM
More information2620 Modular Measurement and Control System
European Union (EU) Council Directive 89/336/EEC Electromagnetic Compatibility (EMC) Test Report 2620 Modular Measurement and Control System Sensoray March 31, 2006 April 4, 2006 Tests Conducted by: ElectroMagnetic
More informationAlternative Coupling Method for Immunity Testing of Power Grid Protection Equipment
Alternative Coupling Method for Immunity Testing of Power Grid Protection Equipment Christian Suttner*, Stefan Tenbohlen Institute of Power Transmission and High Voltage Technology (IEH), University of
More informationA Comparison Between MIL-STD and Commercial EMC Requirements Part 2. By Vincent W. Greb President, EMC Integrity, Inc.
A Comparison Between MIL-STD and Commercial EMC Requirements Part 2 By Vincent W. Greb President, EMC Integrity, Inc. OVERVIEW Compare and contrast military (i.e., MIL-STD) and commercial EMC immunity
More informationINTERNATIONAL STANDARD
INTERNATIONAL STANDARD IEC 61000-2-13 First edition 2005-03 BASIC EMC PUBLICATION Electromagnetic compatibility (EMC) Part 2-13: Environment High-power electromagnetic (HPEM) environments Radiated and
More informationThis is a preview - click here to buy the full publication
TECHNICAL REPORT IEC TR 63170 Edition 1.0 2018-08 colour inside Measurement procedure for the evaluation of power density related to human exposure to radio frequency fields from wireless communication
More informationApplication Note 5525
Using the Wafer Scale Packaged Detector in 2 to 6 GHz Applications Application Note 5525 Introduction The is a broadband directional coupler with integrated temperature compensated detector designed for
More informationINVENTION DISCLOSURE- ELECTRONICS SUBJECT MATTER IMPEDANCE MATCHING ANTENNA-INTEGRATED HIGH-EFFICIENCY ENERGY HARVESTING CIRCUIT
INVENTION DISCLOSURE- ELECTRONICS SUBJECT MATTER IMPEDANCE MATCHING ANTENNA-INTEGRATED HIGH-EFFICIENCY ENERGY HARVESTING CIRCUIT ABSTRACT: This paper describes the design of a high-efficiency energy harvesting
More informationMeasurement and Analysis for Switchmode Power Design
Measurement and Analysis for Switchmode Power Design Switched Mode Power Supply Measurements AC Input Power measurements Safe operating area Harmonics and compliance Efficiency Switching Transistor Losses
More informationEMF Compliance Assessments of 5G Devices
EMF Compliance Assessments of 5G Devices Serge Pfeifer, IT IS Foundation Esra Neufeld, IT IS Foundation Eduardo Carrasco, IT IS Foundation Andreas Christ, IT IS Foundation Myles Capstick, IT IS Foundation
More informationDr. Ali Muqaibel. Associate Professor. Electrical Engineering Department King Fahd University of Petroleum & Minerals Dhahran, Saudi Arabia
By Associate Professor Electrical Engineering Department King Fahd University of Petroleum & Minerals Dhahran, Saudi Arabia Wednesday, December 1, 14 1 st Saudi Symposium for RADAR Technology 9 1 December
More information1000BASE-T1 EMC Test Specification for Common Mode Chokes
IEEE 1000BASE-T1 EMC Test Specification for Common Mode Chokes Version 1.0 Author & Company Dr. Bernd Körber, FTZ Zwickau Title 1000BASE-T1 EMC Test Specification for Common Mode Chokes Version 1.0 Date
More informationModeling and Practical Suggestions to Improve ESD Immunity Test Repeatability
17 th Symposium IMEKO TC, 3 rd Symposium IMEKO TC 19 and 15 th IWDC Workshop Sept. -1, 1, Kosice, Slovakia Modeling and Practical Suggestions to Improve ESD Immunity Test Repeatability. Morando 1, M. Borsero,.
More informationLecture Fundamentals of Data and signals
IT-5301-3 Data Communications and Computer Networks Lecture 05-07 Fundamentals of Data and signals Lecture 05 - Roadmap Analog and Digital Data Analog Signals, Digital Signals Periodic and Aperiodic Signals
More informationContents. 1 Introduction. 2 System-Level Electrostatic Discharge (ESD) and Electrical Fast Transient. 3 Electromagnetic Interference
Issue 3, October 2002 Electromagnetic Compatibility and Electrical Safety Contents Telcordia GR-1089 - Documentation Information Generic Requirements Notice Of Disclaimer................. iii Contents.......................................
More informationTHE PROPAGATION OF PARTIAL DISCHARGE PULSES IN A HIGH VOLTAGE CABLE
THE PROPAGATION OF PARTIAL DISCHARGE PULSES IN A HIGH VOLTAGE CABLE Z.Liu, B.T.Phung, T.R.Blackburn and R.E.James School of Electrical Engineering and Telecommuniications University of New South Wales
More informationEMC Seminar Series All about EMC Testing and Measurement Seminar 1
EMC Seminar Series All about EMC Testing and Measurement Seminar 1 Introduction to EMC Conducted Immunity Jeffrey Tsang Organized by : Department of Electronic Engineering 1 Basic Immunity Standards: IEC
More informationMethods for Testing Impulse Noise Tolerance
Methods for Testing Impulse Noise Tolerance May,6,2015 Larry Cohen Overview Purpose: Describe some potential test methods for impulse noise tolerance What we will cover in this presentation: Discuss need
More informationSCOPE OF ACCREDITATION TO ISO/IEC 17025:2005 AMETEK CO., LTD. NAGOYA OFFICE. (Main Laboratory) Onna, Atsugi-shi, Kanagawa-ken, Japan
SCOPE OF ACCREDITATION TO ISO/IEC 17025:2005 AMETEK CO., LTD. NAGOYA OFFICE (Main Laboratory) 5-1-1 Onna, Atsugi-shi, Kanagawa-ken, 243-0032 Japan (Commercial Office) 1-329 Kifune, Meito-ku Nagoya-shi,
More informationA GTEM BEST PRACTICE GUIDE APPLYING IEC TO THE USE OF GTEM CELLS
- 27-39 H1 A BEST PRACTICE GUIDE APPLYING IEC 61-4-2 TO THE USE OF CELLS A. Nothofer, M.J. Alexander, National Physical Laboratory, Teddington, UK, D. Bozec, D. Welsh, L. Dawson, L. McCormack, A.C. Marvin,
More informationEMC Near-field Probes + Wideband Amplifier
1 Introduction The H20, H10, H5 and E5 are magnetic field (H) and electric field (E) probes for radiated emissions EMC precompliance measurements. The probes are used in the near field of sources of electromagnetic
More information4.4.3 Measurement of the DIFA Against Conducting Boxes of Various Size. Gap
4.4.3 Measurement of the DIFA Against Conducting Boxes of Various Size In Section 4.3.3, the IFA and DIFA were modeled numerically over wire mesh representations of conducting boxes. The IFA was modeled
More informationPicoSource PG900 Series
USB differential pulse generators Three PicoSource models Integrated 60 ps pulse outputs: PG911 Tunnel diode 40 ps pulse heads: PG912 Both output types: PG914 Integrated pulse outputs Differential with
More informationIEC Electrical fast transient / Burst immunity test
CONDUCTED RF EQUIPMENT POWER AMPLIFIERS IEC 61000-4-4 Electrical fast transient / Burst immunity test IEC 61000-4-4 Electrical fast transient / Burst immunity test Markus Fuhrer Phenomenom open a contact
More informationImproving CDM Measurements With Frequency Domain Specifications
Improving CDM Measurements With Frequency Domain Specifications Jon Barth (1), Leo G. Henry Ph.D (2), John Richner (1) (1) Barth Electronics, Inc, 1589 Foothill Drive, Boulder City, NV 89005 USA tel.:
More informationTable of Contents. 1 Introduction. 2 System-Level Electrostatic Discharge (ESD) and Electrical Fast Transient (EFT) 3 Electromagnetic Interference
Electromagnetic Compatibility and Electrical Safety GR-1089-CORE Table of Contents Table of Contents 1 Introduction 1.1 Purpose and Scope.................................. 1 1 1.2 Items Not Covered in
More informationAN IMPROVED MODEL FOR ESTIMATING RADIATED EMISSIONS FROM A PCB WITH ATTACHED CABLE
Progress In Electromagnetics Research M, Vol. 33, 17 29, 2013 AN IMPROVED MODEL FOR ESTIMATING RADIATED EMISSIONS FROM A PCB WITH ATTACHED CABLE Jia-Haw Goh, Boon-Kuan Chung *, Eng-Hock Lim, and Sheng-Chyan
More informationCustom Interconnects Fuzz Button with Hardhat Test Socket/Interposer 1.00 mm pitch
Custom Interconnects Fuzz Button with Hardhat Test Socket/Interposer 1.00 mm pitch Measurement and Model Results prepared by Gert Hohenwarter 12/14/2015 1 Table of Contents TABLE OF CONTENTS...2 OBJECTIVE...
More informationImmunity Testing for the CE Mark
Immunity Testing for the CE Mark Summary The European Union (EU) currently has 25 member countries with 2 additional countries to be added in 2007. The total population at that time will be nearly a half
More informationEMC TEST REPORT For MPP SOLAR INC Inverter/ Charger Model Number : PIP 4048HS
EMC-E20130903E EMC TEST REPORT For MPP SOLAR INC Inverter/ Charger Model Number : PIP 4048HS Prepared for : MPP SOLAR INC Address : 4F, NO. 50-1, SECTION 1, HSIN-SHENG S. RD. TAIPEI, TAIWAN Prepared by
More informationEnvironmental Exposures to ELF Georg Neubauer
Environmental Exposures to ELF Georg Neubauer 1 Table of Content Environmental exposures to ELF sources Measurement methods Requirements on measurements Conclusions 2 Environmental exposure to ELF sources
More informationPredicting Module Level RF Emissions from IC Emissions Measurements using a 1 GHz TEM or GTEM Cell A Review of Related Published Technical Papers 1
Predicting Module Level RF Emissions from IC Emissions Measurements using a 1 GHz TEM or GTEM Cell A Review of Related Published Technical Papers 1 Jame P. Muccioli, Jastech EMC Consulting, LLC, P.O. Box
More informationEFFECT OF INTEGRATION ERROR ON PARTIAL DISCHARGE MEASUREMENTS ON CAST RESIN TRANSFORMERS. C. Ceretta, R. Gobbo, G. Pesavento
Sept. 22-24, 28, Florence, Italy EFFECT OF INTEGRATION ERROR ON PARTIAL DISCHARGE MEASUREMENTS ON CAST RESIN TRANSFORMERS C. Ceretta, R. Gobbo, G. Pesavento Dept. of Electrical Engineering University of
More informationTest Report. Guangdong East Power Co., Ltd. Fully Automatic AC Voltage Regulator. Brand Name:
Test Report Applicant: Product Name: Brand Name: Model No.: Guangdong East Power Co., Ltd. Fully Automatic AC Voltage Regulator EAST ZTY-30KVA Date of Receipt : Aug. 30, 2013 Date of Test: Sep. 03, 2013
More informationAries Kapton CSP socket
Aries Kapton CSP socket Measurement and Model Results prepared by Gert Hohenwarter 5/19/04 1 Table of Contents Table of Contents... 2 OBJECTIVE... 3 METHODOLOGY... 3 Test procedures... 4 Setup... 4 MEASUREMENTS...
More informationSpecification. Patent Pending. Description : AccuraUWB Flex Series 3~10GHz Ultra-Wide Band (UWB) Flex Antenna with 100mm 1.
Specification Patent Pending Part No. : FXUWB10.07.0100C Description : AccuraUWB Flex Series 3~10GHz Ultra-Wide Band (UWB) Flex Antenna with 100mm 1.37mm IPEX MHFHT Features : Flexible UWB Antenna Mounting
More informationTEST REPORT... 1 CONTENT...
CONTENT TEST REPORT... 1 CONTENT... 2 1 TEST RESULTS SUMMARY... 3 2 EMC RESULTS CONCLUSION... 4 3 LABORATORY MEASUREMENTS... 6 4 EMI TEST... 7 4.1 CONTINUOUS CONDUCTED DISTURBANCE VOLTAGE TEST... 7 4.2
More informationA New TEM Horn Antenna Designing Based on Plexiglass Antenna Cap
Journal of Applied Science and Engineering, Vol. 21, No. 3, pp. 413 418 (2018) DOI: 10.6180/jase.201809_21(3).0012 A New TEM Horn Antenna Designing Based on Plexiglass Antenna Cap Lin Teng and Jie Liu*
More informationUtilizzo del Time Domain per misure EMI
Utilizzo del Time Domain per misure EMI Roberto Sacchi Measurement Expert Manager - Europe 7 Giugno 2017 Compliance EMI receiver requirements (CISPR 16-1-1 ) range 9 khz - 18 GHz: A normal +/- 2 db absolute
More informationFilters And Waveform Shaping
Physics 3330 Experiment #3 Fall 2001 Purpose Filters And Waveform Shaping The aim of this experiment is to study the frequency filtering properties of passive (R, C, and L) circuits for sine waves, and
More informationCertificate of Test AND KEEPS ALL REQUIREMENTS ACCORDING THE FOLLOWING REGULATIONS IEC :2001 IEC :2007
Certificate of Test WE HEREBY CERTIFY THAT: Certificate No.: R07122709E Yuan Hsun Electric Co., Ltd. No. 57, Chung He Rd, Zuo-Ying Dist., Kaohsiung City 813, Taiwan R.O.C. Quad photobeam detector Quad-200CS
More informationAC Current Probes CT1 CT2 CT6 Data Sheet
AC Current Probes CT1 CT2 CT6 Data Sheet Features & Benefits High Bandwidth Ultra-low Inductance Very Small Form Factor Characterize Current Waveforms up to
More informationEN 55015: 2013 Clause Pass. EN 55015: 2013 Clause Pass. EN 55015: 2013 Clause Pass
Reference No.: WTD15S0730643E Page 2 of 42 1 Test Summary Test Item Conducted Disturbance at Mains Terminal, 9kHz to 30MHz Radiation electromagnetic disturbance, 9kHz to 30MHz Radiation Emission, 30MHz
More informationMEASUREMENTS OF COUPLING THROUGH BRAIDED SHIELD VIA NEW CONDUCTED IMMUNITY TECH- NIQUE
Progress In Electromagnetics Research C, Vol. 11, 61 68, 2009 MEASUREMENTS OF COUPLING THROUGH BRAIDED SHIELD VIA NEW CONDUCTED IMMUNITY TECH- NIQUE M. Ghassempouri College of Electrical Engineering Iran
More informationGIS Instrument Transformers: EMC Conformity Tests for a Reliable Operation in an Upgraded Substation
GIS Instrument Transformers: EMC Conformity Tests for a Reliable Operation in an Upgraded Substation W. Buesch 1) G. Palmieri M.Miesch J. Marmonier O. Chuniaud ALSTOM LTD 1) ALSTOM LTD High Voltage Equipment
More informationThe EMI/ESD Environment of Large Server Installations
The EMI/ESD Environment of Large Server Installations Douglas C. Smith Mark Hogsett D. C. Smith Consultants Ion Systems, Inc. P. O. Box 1457, Los Gatos, CA 95031 1005 Parker Street, Berkeley, CA 94710
More informationTest and Measurement for EMC
Test and Measurement for EMC Bogdan Adamczyk, Ph.D., in.c.e. Professor of Engineering Director of the Electromagnetic Compatibility Center Grand Valley State University, Michigan, USA Ottawa, Canada July
More informationTransmission Line Pulse Testing and Analysis of Its Influencing Factors
International Conference on Advances in Energy and Environmental Science (ICAEES 2015) Transmission Line Pulse Testing and Analysis of Its Influencing Factors Xue Gu a *and Zhenguang Liang b * School of
More informationUnderstanding Star Switching the star of the switching is often overlooked
A Giga-tronics White Paper AN-GT110A Understanding Star Switching the star of the switching is often overlooked Written by: Walt Strickler V.P. of Business Development, Switching Giga tronics Incorporated
More informationAS/NZS IEC :2013
AS/NZS IEC 61000.4.2:2013 IEC 61000-4-2, Ed.2.0 2008, IDT Australian/New Zealand Standard Electromagnetic compatibility (EMC) Part 4.2: Testing and measurement techniques Electrostatic discharge immunity
More informationImpact of ESD Generator Parameters on Failure Level in Fast CMOS System
Impact of ESD Generator Parameters on Failure Level in Fast CMOS System Abstract Kai Wang, Dr. Pommerenke, Ramachandran Chundru, Jiusheng Huang, Kai Xiao University of Missouri-Rolla EMC laboratory, Rolla,
More informationAgilent E2695A SMA Probe Head for InfiniiMax 1130 Series Active Oscilloscope Probes. User s Guide
User s Guide Publication Number E2695-92000 June 2003 Copyright Agilent Technologies 2003 All Rights Reserved. Agilent E2695A SMA Probe Head for InfiniiMax 1130 Series Active Oscilloscope Probes Agilent
More information4 Investigation of EMC in Wireless Communication Systems
4 Investigation of EMC in Wireless Communication Systems 4-1 Electromagnetic Disturbance Measurement by Using Amplitude Probability Distribution for Protecting Digital Wireless Communication Systems GOTOH
More informationCurrent clamps for AC current
Current clamps for AC current Y series The Y series clamps are designed to be both rugged and versatile whilst remaining easy to use. The jaws are designed so that the clamps can be hooked onto cables
More informationOPEN TEM CELLS FOR EMC PRE-COMPLIANCE TESTING
1 Introduction Radiated emission tests are typically carried out in anechoic chambers, using antennas to pick up the radiated signals. Due to bandwidth limitations, several antennas are required to cover
More informationEMC TEST REPORT. for. Coliy Technology Co.,Ltd. Fluxgate Gaussmeter
Page 1 of 48 EMC TEST REPORT for Coliy Technology Co.,Ltd. Fluxgate Gaussmeter Prepared for : Coliy Technology Co.,Ltd. Address : Block B,9 th Floor,Xinzhongtai Business Building,Gushu 2nd Road,Xi Town,Bao
More informationCoherence and time-frequency analysis of impulse voltage and current measurements
Coherence and time-frequency analysis of impulse voltage and current measurements Jelena Dikun Electrical Engineering Department, Klaipeda University, Klaipeda, Lithuania Emel Onal Electrical Engineering
More informationRCTrms Technical Notes
RCTrms Technical Notes All measuring instruments are subject to limitations. The purpose of these technical notes is to explain some of those limitations and to help the engineer maximise the many advantages
More informationAn Introduction to Spectrum Analyzer. An Introduction to Spectrum Analyzer
1 An Introduction to Spectrum Analyzer 2 Chapter 1. Introduction As a result of rapidly advancement in communication technology, all the mobile technology of applications has significantly and profoundly
More information6 - Stage Marx Generator
6 - Stage Marx Generator Specifications - 6-stage Marx generator has two capacitors per stage for the total of twelve capacitors - Each capacitor has 90 nf with the rating of 75 kv - Charging voltage used
More informationSystem description 4. SERVICES ONSITE INSTALLATION AND TRAINING SYSTEM ACCEPTANCE MAINTENANCE... 7
Ultra Wide Band test setup System description 1. UWB TEST SYSTEM DESCRIPTION... 2 2. SYSTEM MONITORING... 5 3. OTHER MEASUREMENT SYSTEMS & ACCESSORIES... 6 3.1 OSCILLOSCOPE & SHIELDED ENCLOSURE... 6 3.2
More informationSources of transient electromagnetic disturbance in medium voltage switchgear
Sources of transient electromagnetic disturbance in medium voltage switchgear Dennis Burger, Stefan Tenbohlen, Wolfgang Köhler University of Stuttgart Stuttgart, Germany dennis.burger@ieh.uni-stuttgart.de
More informationMulti-Resolution Wavelet Analysis for Chopped Impulse Voltage Measurements
Multi-Resolution Wavelet Analysis for Chopped Impulse Voltage Measurements EMEL ONAL Electrical Engineering Department Istanbul Technical University 34469 Maslak-Istanbul TURKEY onal@elk.itu.edu.tr http://www.elk.itu.edu.tr/~onal
More informationOverview of the ATLAS Electromagnetic Compatibility Policy
Overview of the ATLAS Electromagnetic Compatibility Policy G. Blanchot CERN, CH-1211 Geneva 23, Switzerland Georges.Blanchot@cern.ch Abstract The electromagnetic compatibility of ATLAS electronic equipments
More informationPicoSource PG900 Series USB differential pulse generators
USB differential pulse generators Three PicoSource models Integrated 60 ps pulse outputs: PG911 Tunnel diode 40 ps pulse heads: PG912 Both output types: PG914 Integrated pulse outputs Differential with
More informationEN 55022: 2010+AC:2011 Clause 6.1 Pass. Harmonic Current EN :2006+A1:2009+A2:2009 Class A N/A
Reference No.: WT12106773-N-S-E Page 2 of 33 1 Test Summary Test Item Mains Terminal Disturbance Voltage, 150KHz to 30MHz Radiation Emission, 30MHz to 1000MHz EMISSION Test Standard Class / Severity Result
More informationEN :2007+A1:2011 Electromagnetic compatibility Emission standard for residential, commercial and light-industrial environments
EMC Page 3 / 33 Test report No.: EN 61000-6-3:2007+A1:2011 Electromagnetic compatibility Emission standard for residential, commercial and light-industrial environments Date of measurement: 2013-10-16
More information10 GHz Microwave Link
10 GHz Microwave Link Project Project Objectives System System Functionality Testing Testing Procedures Cautions and Warnings Problems Encountered Recommendations Conclusion PROJECT OBJECTIVES Implement
More informationFISCHER CUSTOM COMMUNICATIONS, INC.
FISCHER CUSTOM COMMUNICATIONS, INC. Current Probe Catalog FISCHER CUSTOM COMMUNICATIONS, INC. Fischer Custom Communications, Inc., is a manufacturer of custom electric and magnetic field sensors for military
More informationModelling electromagnetic field coupling from an ESD gun to an IC
Modelling electromagnetic field coupling from an ESD gun to an IC Ji Zhang #1, Daryl G Beetner #2, Richard Moseley *3, Scott Herrin *4 and David Pommerenke #5 # EMC Laboratory, Missouri University of Science
More information2310 to 2390 MHz, 3m distance MCS8 (MIMO) to 2500 MHz Restricted band MCS8 (MIMO)
2310 to 2390 MHz, 3m distance MCS8 (MIMO) Lower band edge, Average (Low Channel) Lower band edge, Peak (Low Channel) 2483.5 to 2500 MHz Restricted band MCS8 (MIMO) Upper band edge, Peak (High Channel)
More informationOverview of EMC Regulations and Testing. Prof. Tzong-Lin Wu Department of Electrical Engineering National Taiwan University
Overview of EMC Regulations and Testing Prof. Tzong-Lin Wu Department of Electrical Engineering National Taiwan University What is EMC Electro-Magnetic Compatibility ( 電磁相容 ) EMC EMI (Interference) Conducted
More informationTest Report GUANGDONG EAST POWER CO., LTD
Test Report Applicant: Product Name: Brand Name: Model No.: GUANGDONG EAST POWER CO., LTD Online High Frequency UPS EAST EA906IIRTS, EA906IIRTH Date of Receipt : Feb. 26, 2014 Date of Test: Mar. 24, 2014
More information150Hz to 1MHz magnetic field coupling to a typical shielded cable above a ground plane configuration
150Hz to 1MHz magnetic field coupling to a typical shielded cable above a ground plane configuration D. A. Weston Lowfreqcablecoupling.doc 7-9-2005 The data and information contained within this report
More informationTLP/VF-TLP/HMM Test System TLP-3010C/3011C Advanced TLP/HMM/HBM Solutions
1 Features Wafer and package level TLP/VF-TLP/HMM testing Ultra fast high voltage pulse output with typical 1 ps rise time Built-in HMM (IEC 61-4-2) pulse up to ±8 kv High pulse output current up to ±3
More informationBS EN TESTS ON THE IT TOXIC GAS DETECTOR MODULE
Page 1 of 18 Interference Testing And Consultancy Services (Pty) Ltd ITC SERVICES (PTY) LTD Reg 88/002032/07 Plot 44 Kameeldrift East, Pretoria Private Bag X13 Lynn East 0039 Republic of South Africa Tel
More informationFlexible AC current probes
Flexible AC current probes Making use of the principle of Rogowski coils, the MiniFLEX models are flexible sensors offering a wide dynamic range for measuring AC intensities and viewing high-speed current
More informationANTENNA INTRODUCTION / BASICS
ANTENNA INTRODUCTION / BASICS RULES OF THUMB: 1. The Gain of an antenna with losses is given by: 2. Gain of rectangular X-Band Aperture G = 1.4 LW L = length of aperture in cm Where: W = width of aperture
More informationP331-2 set ESD generator (IEC )
User manual Probe set set ESD generator (IEC 61000-4-2) Copyright January 2017 LANGER GmbH 2017.01.09 User manual Table of contents: Page 1 ESD generator (IEC 61000-4-2) 3 1.1 Design and function of the
More informationSCOPE OF ACCREDITATION TO ISO/IEC 17025:2005
SCOPE OF ACCREDITATION TO ISO/IEC 17025:2005 JEL LIMITED 2971 Nakabyo, Abiko-City Chiba-Prefecture, 270-1121, JAPAN Keiichiro Murata Phone: +81 4 7188 5333 Email: murata@jel.co.jp CALIBRATION Valid To:
More informationTime Domain Reflectometry (TDR) and Time Domain Transmission (TDT) Measurement Fundamentals
Time Domain Reflectometry (TDR) and Time Domain Transmission (TDT) Measurement Fundamentals James R. Andrews, Ph.D., IEEE Fellow PSPL Founder & former President (retired) INTRODUCTION Many different kinds
More informationOPEN TEM CELLS FOR EMC PRE-COMPLIANCE TESTING
1 Introduction Radiated emission tests are typically carried out in anechoic chambers, using antennas to pick up the radiated signals. Due to bandwidth limitations, several antennas are required to cover
More informationMhow (MP) PIN c/o 56 APO RFI : PROCUREMENT OF FAST TRANSIENT RESPONSE ELECTROMAGNETIC PULSE (EMP) SIMULATOR
Tele : 07324-256130 Army Centre for Electromagnetics Mhow (MP) PIN - 900444 c/o 56 APO 2710/M/EMP Sml/ 23 Jul 20 To RFI : PROCUREMENT OF FAST TRANSIENT RESPONSE ELECTROMAGNETIC PULSE (EMP) SIMULATOR 1.
More information